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Poster Abstracts - Kepler - NASA

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POSTER ABSTRACTSP0403. POSTER SESSION ITHERMAL EVOLUTION AND MASS LOSS OF WATER-RICH SUPER-EARTHS. K. Kurosaki 1 , M. Ikoma1 , Y. Hori 2 and S. Ida 1 1 Department of Earth and Planetary Sciences, Tokyo Institute of Technology, Ookayama,Meguro-ku, Tokyo 152-8551, Japan; kurosaki@geo.titech.ac.jp (K. K.), mikoma@geo.titech.ac.jp (M. I.),ida@geo.titech.ac.jp (S. I.). 2 Division of Theoretical Astronomy, National Astronomical Observatory of Japan,Osawa, Mitaka, Tokyo, 181-8588, Japan; yasunori.hori@geo.titech.ac.jp .Introduction: Recent progresses in transit photometry—especially,operation of the two space-basedtelescope <strong>Kepler</strong> and CoRoT—have enabled us to findrelatively small short-period exoplanets with radii of afew to several Earth radii. Combined with planerarymasses measured by radial-velocity or transit-timingvariationmethods, many of the planets and planetarycandidates are inferred to be water-rich objects likeUranus and Neptune. Such objects are often called hotNeprunes. The radii of hot Neptunes are relatively sensitiveto their thermal and gravitational energy. Thus,understanding the distribution of hot Neptunes in themass-radius (or bulk density) diagram gives us greatinsights into the formation and evolution of the planetswhich include the histories of accretion, impact/erosion,and loss of energy and mass.Similarly to gas giants, water-dominanted planetsare born big in size. Then they shrink or become denserlosing their accrerion energy into space. Furthermore,since transiting planets orbit close to their hoststars, they experience mass loss driven by intense stellarX-ray and UV irradiation (XUV). Thus, interestingquestions are how large is the maximum radius (or theminimum bulk density) of a hot Neptune of a givenmass that we observe and how large is the minimummass of a hot Neptune that survives the mass loss.Previously, the thermal evolution and mass loss ofhot-Jupiters were investigated [1,2]. The mass andradius relationships of water-rich planets were calculatedfor relatively wide ranges of intrinsic and equilibriumtemperatures by Rogers et al. (2011) and Valenciaet al. (2010); they also estimated the possibleamounts of mass loss [3,4]. However, to ourknowledge, there is no study that simulates the thermalevolution and mass loss of water-rich planets concurrently.Methods: In this study, we have simulated thespherically symmetric structure and thermal evolutionof planets that are composed mainly of water. Themass loss is assumed to be due to stellar XUV irradiation;the mass loss rate is calculated, based on theoryof the energy limited hydrodynamic escape through theRoche lobe of the planet. The structure of the atmosphereis integrated, following Guillot (2010) [5].Results: The planet gets cold and shrinks by emittingits intrinsic heat. Inside the planet, the boundarybetween the radiative and convective layers becomesdeeper and deeper. This controls the thermal evolution.On a timescale of 1-10 Gyr, the intrinsic temperaturedecreases to a few ten Kelvin. At that time, the radiiare several to ten Earth radii for 1-10 Earth-mass water-dominatedplanets, provided the mass loss is ignored.However, if the mass loss is included, the lowmassand large-radius planets evaporate completely.Since the stellar XUV declines and the planetary radiusbecomes small with time, we have found there are distinctthreshold masses beyond which the planet survivesthe evporation due to XUV irradiation from thehost star. While the threshold mass depends on severalproperties of the planet and the star, it is found to bearound 10 Earth masses.Conclusions: We have found that the thermal evolutionof water-rich planets has a significant impact ontheir radius and mass loss rate. Besides, there is thelower limit to the mass of the planet that survives themass loss due to XUV irradiation from the host starsfor 10 billion years. These results give constraints tothe distribution of water-rich super-Earths on the massradius(or bulk density) diagram.References: [1] Baraffe, I. et al. (2003) A&A, 402,701-712. [2] Yelle, R. (2004) Icarus, 170, 167-179.[3] Rogers, L. et al. (2011) ApJ, 738, 59. [4] Valencia,D. et al. (2010) A&A, 516, A20. [5]Guillot,T. (2010)A&A, 520, A27.1622011 <strong>Kepler</strong> Science Conference - <strong>NASA</strong> Ames Research Center

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