2012A&A...547A.112M


Query : 2012A&A...547A.112M

2012A&A...547A.112M - Astronomy and Astrophysics, volume 547A112-112 (2012/11-1)

Characterization of exoplanets from their formation. II. The planetary mass-radius relationship.

MORDASINI C., ALIBERT Y., GEORGY C., DITTKRIST K.-M., KLAHR H. and HENNING T.

Abstract (from CDS):

The research of extrasolar planets has entered an era in which we characterize extrasolar planets. This has become possible with measurements of the radii of transiting planets and of the luminosity of planets observed by direct imaging. Meanwhile, the precision of radial velocity surveys makes it possible to discover not only giant planets but also very low-mass ones. Uniting all these different observational constraints into one coherent picture to better understand planet formation is an important and simultaneously difficult undertaking. One approach is to develop a theoretical model that can make testable predictions for all these observational techniques. Our goal is to have such a model and use it in population synthesis calculations. In a companion paper, we described how we have extended our formation model into a self-consistently coupled formation and evolution model. In this second paper, we first continue with the model description. We describe how we calculate the internal structure of the solid core of the planet and include radiogenic heating. We also introduce an upgrade of the protoplanetary disk model. Finally, we use the upgraded model in population synthesis calculations. We present how the planetary mass-radius relationship of planets with primordial H2/He envelopes forms and evolves in time. The basic shape of the mass-radius relationship can be understood from the core accretion model. Low-mass planets cannot bind massive envelopes, while super-critical cores necessarily trigger runway gas accretion, leading to ``forbidden'' zones in the M-R plane. For a given mass, there is a considerable diversity of radii, mainly due to different bulk compositions, reflecting different formation histories. We compare the synthetic M-R plane with the observed one, finding good agreement for a>0.1AU. The synthetic planetary radius distribution is characterized by a strong increase towards small R and a second, lower local maximum at about 1 ⊕. The increase towards small radii comes from the increase of the mass function towards low M. The second local maximum is due to the fact that radii are nearly independent of mass for giant planets. A comparison of the synthetic radius distribution with Kepler data shows good agreement for R>2R⊕, but divergence for smaller radii. This indicates that for R>2R⊕ the radius distribution can be described with planets with primordial H2/He atmospheres, while at smaller radii, planets of a different nature dominate. We predict that in the next few years, Kepler will find the second local maximum at about 1 ⊕. With the updated model, we can compute the most important quantities, like mass, semimajor axis, radius, and luminosity, which characterize an extrasolar planet self-consistently from its formation. The comparison of the radii of the synthetic planets with observations makes it possible to better constrain this formation process and to distinguish between fundamental types of planets.

Abstract Copyright: ∼

Journal keyword(s): planetary systems - planet-disk interactions - planets and satellites: formation - planets and satellites: interiors - planets and satellites: individual: Jupiter - methods: numerical

Simbad objects: 29

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Number of rows : 29
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 17156b Pl 02 49 44.4871034544 +71 45 11.629235988           ~ 197 1
2 NAME Ori Trapezium OpC 05 35 16.5 -05 23 14           ~ 1708 1
3 CoRoT-7b Pl 06 43 49.4690164104 -01 03 46.826642700           ~ 422 1
4 HD 80606b Pl 09 22 37.5768032712 +50 36 13.435326684           ~ 369 1
5 Ross 905b Pl 11 42 11.0933350978 +26 42 23.650782778           ~ 913 1
6 * rho Oph ** 16 25 35.11766 -23 26 49.8150 4.30 4.85 4.63 4.27 3.96 B2IV+B2V 670 0
7 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3969 1
8 NAME G 139-21b Pl 17 15 18.9339850845 +04 57 50.066612336           ~ 845 1
9 CoRoT-9b Pl 18 43 08.8100358120 +06 12 14.913236808           ~ 73 1
10 Kepler-30 Er* 19 01 08.0746104528 +38 56 50.218268856   16.50   15.767 14.55 ~ 180 1
11 Kepler-9c Pl 19 02 17.7544327200 +38 24 03.176851896           ~ 109 1
12 Kepler-9b Pl 19 02 17.7544327200 +38 24 03.176851896           ~ 121 1
13 Kepler-10b Pl 19 02 43.0613892904 +50 14 28.701617339           ~ 322 1
14 Kepler-10c Pl 19 02 43.0613892904 +50 14 28.701617339           ~ 135 1
15 Kepler-10 Em* 19 02 43.0613892904 +50 14 28.701617339       11.00   G2V 238 1
16 Kepler-20 Er* 19 10 47.5233433920 +42 20 19.301370684   13.278 12.630 12.478 11.64 G5V 201 1
17 Kepler-20d Pl 19 10 47.5233433920 +42 20 19.301370684           ~ 77 1
18 Kepler-16b Pl 19 16 18.1758378936 +51 45 26.782726104           ~ 178 1
19 CoRoT-10b Pl 19 24 15.2869439208 +00 44 46.002641280           ~ 61 1
20 Kepler-35b Pl 19 37 59.2726213344 +46 41 22.952695956           ~ 99 1
21 Kepler-34b Pl 19 45 44.5974898536 +44 38 29.610983076           ~ 115 1
22 Kepler-39b Pl 19 47 50.4745594512 +46 02 03.499726272           ~ 73 1
23 Kepler-11f Pl 19 48 27.6226218768 +41 54 32.903163504           ~ 139 1
24 Kepler-11d Pl 19 48 27.6226218768 +41 54 32.903163504           ~ 131 1
25 Kepler-11e Pl 19 48 27.6226218768 +41 54 32.903163504           ~ 134 1
26 Kepler-11 Er* 19 48 27.6226218768 +41 54 32.903163504   14.635 13.838 13.742   G2V 377 1
27 Kepler-11g Pl 19 48 27.6226218768 +41 54 32.903163504           ~ 85 1
28 Kepler-11c Pl 19 48 27.6226218768 +41 54 32.903163504           ~ 119 1
29 Kepler-18d Pl 19 52 19.0688312520 +44 44 46.807928916           ~ 90 1

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