2026ApJ...996...12K


Query : 2026ApJ...996...12K

2026ApJ...996...12K - Astrophys. J., 996, 12 (2026/January-1)

Higher-order Mean-motion Resonances Can Form in Type I Disk Migration.

KELLER F.M., DAI F. and XU W.

Abstract (from CDS):

Type I disk migration can form a chain of planets engaged in first-order mean-motion resonances (MMRs) parked at the disk inner edge. However, while second- or even third-order resonances were deemed unlikely due to their weaker strength, they have been observed in some planetary systems, e.g., TOI-178 bc (5:3), TOI-1136 ef (7:5), and TRAPPIST-1 bcd (8:5-5:3). We performed >6000 Type I simulations of multiplanet systems that mimic the observed Kepler sample in terms of stellar mass, planet size, multiplicity, and intra-system uniformity over a parameter space encompassing transitional and truncated disks. We found that Type I migration coupled with a disk inner edge can indeed produce second- and third-order resonances (in a state of libration) in ∼10% and 2% of resonant-chain systems, respectively. Moreover, the relative occurrence of first- and second-order MMRs in our simulations is consistent with observations (e.g., 3:2 is more common than 2:1; while second-order 5:3 is more common than 7:5). The formation of higher-order MMRs favors slower disk migration and a smaller outer planet mass. Higher-order resonances do not have to form with the help of a Laplace-like three-body resonance, as was proposed for TRAPPIST-1. Instead, the formation of higher-order resonances is assisted by breaking a preexisting first-order resonance, which generates small but nonzero initial eccentricities (e ≈ 10–3 to 10–2). We predict that (1) librating higher-order resonances have higher equilibrium e (∼0.1), (2) are more likely found as an isolated pair in an otherwise first-order chain, and (3) more likely emerge in the inner pairs of a chain.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Exoplanet formation - Exoplanet dynamics - N-body simulations - Modified Newtonian dynamics - Celestial mechanics - Orbits

Simbad objects: 19

goto Full paper

goto View the references in ADS

Number of rows : 19
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-178c Pl 00 29 12.3029193648 -30 27 13.466857032           ~ 29 0
2 TOI-178b Pl 00 29 12.3029193648 -30 27 13.466857032           ~ 29 0
3 BD+65 902 MS* 12 48 44.3726123832 +64 51 19.147528800   10.16 9.53     G5 50 0
4 BD+65 902f Pl 12 48 44.3726123832 +64 51 19.147528800           ~ 9 0
5 BD+65 902e Pl 12 48 44.3726123832 +64 51 19.147528800           ~ 8 0
6 Kepler-138e Pl 19 21 31.5679755816 +43 17 34.680970608           ~ 8 0
7 Kepler-138d Pl 19 21 31.5679755816 +43 17 34.680970608           ~ 86 0
8 Kepler-138c Pl 19 21 31.5679755816 +43 17 34.680970608           ~ 80 0
9 Kepler-36b Pl 19 25 00.0428079600 +49 13 54.630900876           ~ 163 1
10 Kepler-36c Pl 19 25 00.0428079600 +49 13 54.630900876           ~ 133 1
11 Kepler-29c Pl 19 53 23.6017612992 +47 29 28.436776467           ~ 45 1
12 Kepler-29b Pl 19 53 23.6017612992 +47 29 28.436776467           ~ 52 1
13 TRAPPIST-1d Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 263 0
14 TRAPPIST-1 LM* 23 06 29.3684948589 -05 02 29.037301866     18.798 16.466 14.024 M7.5e 1306 0
15 TRAPPIST-1b Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 380 0
16 TRAPPIST-1c Pl 23 06 29.3684948589 -05 02 29.037301866           ~ 282 0
17 K2-138g Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 12 0
18 K2-138f Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 22 0
19 K2-138e Pl 23 15 47.7686067840 -10 50 58.895461284           ~ 22 0

To bookmark this query, right click on this link: simbad:objects in 2026ApJ...996...12K and select 'bookmark this link' or equivalent in the popup menu