2023A&A...677A.160C


Query : 2023A&A...677A.160C

2023A&A...677A.160C - Astronomy and Astrophysics, volume 677A160 (2023/9-1)

Tidal interactions shape period ratios in planetary systems with three-body resonant chains.

CHARALAMBOUS C., TEYSSANDIER J. and LIBERT A.-S.

Abstract (from CDS):

Aims. These last years several STIPs (Systems with Tightly packed Inner Planets) in the super-Earth mass regime have been discovered harboring chains of resonances. It is generally believed that planet pairs get trapped in MMR (mean-motion resonance) during the migration phase in the protoplanetary disk, while the tides raised by the host star provide a source of dissipation on very long timescales. In this work, we aim to study the departure from exact commensurabilities observed among the STIPs which harbor 3-planet resonances and analyze how tides play an important role in shaping the resonance offsets for the STIPs.
Methods. We analyzed the resonance offsets between adjacent pairs for five multi-planetary systems, namely Kepler-80, Kepler-223, K2-138, TOI-178, and TRAPPIST-1, highlighting the existence of different trends in the offsets. On the one hand, we derived analytical estimates for the offsets, which confirm that the departure of the planetary pairs from the nominal MMRs are due to the 3-planet resonant dynamics. On the other hand, we performed N-body simulations including both orbital migration and tidal dissipation from the host star with simple prescriptions in order to test the effectiveness of this mechanism at shaping the observed trend in the offsets, focusing our study on the preservation of the resonant patterns in the different systems with the same general setup.
Results. We found that the trends in the offsets of the five detected systems can be produced by tidal damping effects, regardless of the considered value for the tidal factor. It is a robust mechanism that relaxes the system towards equilibrium while efficiently moving it along 3-planet resonances, which induces the observed resonance offset for each planet pair. In addition, we showed that for Kepler-80, K2-138, and TOI-178, the amplitudes of the resonant offsets can also be reproduced with an appropriate tidal factor, for the estimated age of the systems.

Abstract Copyright: © The Authors 2023

Journal keyword(s): planets and satellites: physical evolution - planets and satellites: dynamical evolution and stability - planet-star interactions - methods: numerical

Simbad objects: 40

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Number of rows : 40
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 TOI-178b Pl 00 29 12.3029193648 -30 27 13.466857032           ~ 29 0
2 TOI-178e Pl 00 29 12.3029193648 -30 27 13.466857032           ~ 13 0
3 TOI-178g Pl 00 29 12.3029193648 -30 27 13.466857032           ~ 17 0
4 WT 2353 PM* 00 29 12.3029193648 -30 27 13.466857032   13.05 11.95     ~ 102 0
5 TOI-178f Pl 00 29 12.3029193648 -30 27 13.466857032           ~ 15 0
6 TOI-178d Pl 00 29 12.3029193648 -30 27 13.466857032           ~ 20 0
7 TOI-178c Pl 00 29 12.3029193648 -30 27 13.466857032           ~ 29 0
8 HD 158259 PM* 17 25 24.0552880944 +52 47 26.469887928   7.07 6.47     G5VmF9 79 0
9 Kepler-60 Er* 19 15 50.6983640712 +42 15 54.050260968   14.477 14.083 13.934   G2 132 1
10 Kepler-80 Er* 19 44 27.0200680656 +39 58 43.594100688   16.303 15.201 14.866   M0V 177 1
11 Kepler-80g Pl 19 44 27.0200680656 +39 58 43.594100688           ~ 15 0
12 Kepler-80f Pl 19 44 27.0200680656 +39 58 43.594100688           ~ 36 1
13 Kepler-80b Pl 19 44 27.0200680656 +39 58 43.594100688           ~ 52 1
14 Kepler-80e Pl 19 44 27.0200680656 +39 58 43.594100688           ~ 49 1
15 Kepler-80c Pl 19 44 27.0200680656 +39 58 43.594100688           ~ 50 1
16 Kepler-80d Pl 19 44 27.0200680656 +39 58 43.594100688           ~ 54 1
17 Kepler-228 Er* 19 45 08.6682832944 +48 13 28.801638660   16.756 15.909 15.908   ~ 48 0
18 Kepler-221 Er* 19 46 37.1434561728 +46 50 06.841651128   14.853 14.017 13.778   G5 97 0
19 Kepler-223c Pl 19 53 16.4202435936 +47 16 46.308434088           ~ 37 0
20 Kepler-223d Pl 19 53 16.4202435936 +47 16 46.308434088           ~ 48 0
21 Kepler-223e Pl 19 53 16.4202435936 +47 16 46.308434088           ~ 42 0
22 Kepler-223b Pl 19 53 16.4202435936 +47 16 46.308434088           ~ 37 0
23 Kepler-223 Er* 19 53 16.4202435936 +47 16 46.308434088   16.209 15.570 15.78   ~ 192 1
24 BD-15 6290 BY* 22 53 16.7325836486 -14 15 49.304052185 12.928 11.749 10.192 9.013 7.462 M3.5V 1106 1
25 TRAPPIST-1h Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 162 0
26 TRAPPIST-1 LM* 23 06 29.3684948589 -05 02 29.037301866     18.798 16.466 14.024 M7.5e 1306 0
27 TRAPPIST-1c Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 282 0
28 TRAPPIST-1e Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 384 0
29 TRAPPIST-1g Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 237 0
30 TRAPPIST-1b Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 380 0
31 TRAPPIST-1d Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 263 0
32 TRAPPIST-1f Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 281 0
33 HD 218396 El* 23 07 28.7157209544 +21 08 03.310767492   6.21 5.953     F0+VkA5mA5 1285 0
34 K2-138c Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 19 0
35 K2-138g Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 12 0
36 K2-138b Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 18 0
37 K2-138e Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 22 0
38 K2-138f Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 22 0
39 K2-138d Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 22 0
40 K2-138 * 23 15 47.7686067840 -10 50 58.895461284   13.01 12.21 12.12 11.40 ~ 75 0

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