2021A&A...645A..79S


Query : 2021A&A...645A..79S

2021A&A...645A..79S - Astronomy and Astrophysics, volume 645A, 79-79 (2021/1-1)

Evidence of three mechanisms explaining the radius anomaly of hot Jupiters.

SARKIS P., MORDASINI C., HENNING T., MARLEAU G.D. and MOLLIERE P.

Abstract (from CDS):


Context. The anomalously large radii of hot Jupiters are still not fully understood, and all of the proposed explanations are based on the idea that these close-in giant planets possess hot interiors. Most of the mechanisms proposed have been tested on a handful of exoplanets.
Aims. We approach the radius anomaly problem by adopting a statistical approach. We want to infer the internal luminosity for the sample of hot Jupiters, study its effect on the interior structure, and put constraints on which mechanism is the dominant one.
Methods. We developed a flexible and robust hierarchical Bayesian model that couples the interior structure of exoplanets to the observed properties of close-in giant planets. We applied the model to 314 hot Jupiters and inferred the internal luminosity distribution for each planet and studied at the population level (i) the mass-luminosity-radius distribution and as a function of equilibrium temperature the distributions of the (ii) heating efficiency, (iii) internal temperature, and the (iv) pressure of the radiative-convective-boundary (RCB).
Results. We find that hot Jupiters tend to have high internal luminosity with 104LJ for the largest planets. As a result, we show that all the inflated planets have hot interiors with an internal temperature ranging from 200 up to 800K for the most irradiated ones. This has important consequences on the cooling rate and we find that the RCB is located at low pressures between 3 and 100 bar. Assuming that the ultimate source of the extra heating is the irradiation from the host star, we also illustrate that the heating efficiency increases with increasing equilibrium temperature and reaches a maximum of 2.5% at ∼1860K, beyond which the efficiency decreases, which is in agreement with previous results. We discuss our findings in the context of the proposed heating mechanisms and illustrate that ohmic dissipation, the advection of potential temperature, and thermal tides are in agreement with certain trends inferred from our analysis and thus all three models can explain various aspects of the observations.
Conclusions. We provide new insights on the interior structure of hot Jupiters and show that with our current knowledge, it is still challenging to firmly identify the universal mechanism driving the inflated radii.

Abstract Copyright: © P. Sarkis et al. 2021

Journal keyword(s): planets and satellites: gaseous planets - planets and satellites: interiors - planets and satellites: physical evolution

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 HD 10069b Pl 01 37 25.0332798696 -45 40 40.374717456           ~ 369 1
2 WASP-12b Pl 06 30 32.7966092352 +29 40 20.263502460           ~ 762 1
3 CoRoT-4b Pl 06 48 46.7134456728 -00 40 21.969631416           ~ 67 1
4 CD-38 3220b Pl 07 10 24.0604565856 -39 05 50.571250476           ~ 296 0
5 HAT-P-20 PM* 07 27 39.9488720808 +24 20 11.516231112   12.58 11.35 11.00   K3V 73 1
6 K2-114b Pl 08 31 31.9126771776 +11 55 20.156367180           ~ 14 0
7 WASP-43 PM* 10 19 38.0088913464 -09 48 22.605801336   13.782 12.490 12.022 11.10 K7V 148 2
8 Qatar 2 PM* 13 50 37.4100326640 -06 48 14.421574044   14.0   13.45   K5V 67 1
9 BD+36 2955 * 17 50 33.7175464920 +36 34 12.805037904   11.19 10.59   9.998 ~ 13 0
10 TrES-4 Pl 17 53 13.0489562760 +37 12 42.586493328           ~ 214 2
11 TOI-1628b Pl 19 24 38.9614451424 +55 28 23.332107108           ~ 55 1
12 HATS-35b Pl 19 46 45.1812364536 -63 33 56.136897468           ~ 20 0
13 HD 189733b Pl 20 00 43.7129433648 +22 42 39.073143456           ~ 1432 1
14 HAT-P-17b Pl 21 38 08.7310010424 +30 29 19.446386748           ~ 82 1
15 HD 209458b Pl 22 03 10.7727465312 +18 53 03.549393384           ~ 1856 1
16 K2-60 * 22 34 25.4865325464 -13 43 54.159635424   13.56 12.79     ~ 22 0

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