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A&A 506, 399-410 (2009)
DOI: 10.1051/0004-6361/200911922
Determining the mass loss limit for close-in exoplanets: what can we learn from transit observations?
H. Lammer1, P. Odert2, M. Leitzinger2, M. L. Khodachenko1, M. Panchenko1, Yu. N. Kulikov3, T. L. Zhang1, H. I. M. Lichtenegger1, N. V. Erkaev4, G. Wuchterl5, G. Micela6, T. Penz6, 7, H. K. Biernat1, J. Weingrill1, M. Steller1, H. Ottacher1, J. Hasiba1, and A. Hanslmeier21 Space Research Institute, Austrian Academy of Sciences, Schmiedlstrasse 6, 8042 Graz, Austria
e-mail: helmut.lammer@oeaw.ac.at
2 Institute for Physics, IGAM, University of Graz, Universitätsplatz 3, 8010 Graz, Austria
3 Polar Geophysical Institute, Russian Academy of Sciences, Khalturina 15, 183010 Murmansk, Russian Federation
4 Institute for Computational Modelling, Russian Academy of Sciences, and Siberian Federal University, Krasnoyarsk, Russian Federation
5 Thüringer Landessternwarte Tautenburg, Sternwarte 5 07778 Tautenburg, Germany
6 INAF – Osservatorio Astronomico, Piazza del Parlamento 1, 90134 Palermo, Italy
7 On leave from the INAF – Osservatorio Astronomico, Palermo, Italy
Received 23 February 2009 / Accepted 31 July 2009
Abstract
Aims. We study the possible atmospheric mass loss from 57 known transiting exoplanets around F, G, K, and M-type stars over evolutionary timescales. For stellar wind induced mass loss studies, we estimate the position of the pressure balance boundary between Coronal Mass Ejection (CME) and stellar wind ram pressures and the planetary ionosphere pressure for non- or weakly magnetized gas giants at close orbits.
Methods. The thermal mass loss of atomic hydrogen is calculated by a mass loss equation where we consider a realistic heating efficiency, a radius-scaling law and a mass loss enhancement factor due to stellar tidal forces. The model takes into account the temporal evolution of the stellar EUV flux by applying power laws for F, G, K, and M-type stars. The planetary ionopause obstacle, which is an important factor for ion pick-up escape from non- or weakly magnetized gas giants is estimated by applying empirical power-laws.
Results. By assuming a realistic heating efficiency of about 10–25% we found that WASP-12b may have lost about 6–12% of its mass during its lifetime. A few transiting low density gas giants at similar orbital location, like WASP-13b, WASP-15b, CoRoT-1b or CoRoT-5b may have lost up to 1–4% of their initial mass. All other transiting exoplanets in our sample experience negligible thermal loss (
1%) during their lifetime. We found that the ionospheric pressure can balance the impinging dense stellar wind and average CME plasma flows at distances which are above the visual radius of “Hot Jupiters”, resulting in mass losses <2% over evolutionary timescales. The ram pressure of fast CMEs cannot be balanced by the ionospheric plasma pressure for orbital distances between 0.02–0.1 AU. Therefore, collisions of fast CMEs with hot gas giants should result in large atmospheric losses which may influence the mass evolution of gas giants with masses <
. Depending on the stellar luminosity spectral type, planetary density, heating efficiency, orbital distance, and the related Roche lobe effect, we expect that at distances between 0.015–0.02 AU, Jupiter-class and sub-Jupiter-class exoplanets can lose several percent of their initial mass. At orbital distances
0.015 AU, low density hot gas giants in orbits around solar type stars may even evaporate down to their coresize, while low density Neptune-class objects can lose their hydrogen envelopes at orbital distances
0.02 AU.
Key words: planetary systems -- planetary systems: formation
© ESO 2009
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