Amplifying Resonant Repulsion with Inflated Young Planets, Overlooked Inner Planets, and Nonzero Initial Δ

Most multiplanet systems around mature (∼5 Gyr old) host stars are nonresonant. Even the near-resonant planet pairs still display 1%–2% positive deviation from perfect period commensurabilities (Δ) near first-order mean motion resonances (MMRs). Resonant repulsion due to eccentricity tides was one o...

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Main Authors: Yuancheng Xu, Fei Dai
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:The Astrophysical Journal
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Online Access:https://doi.org/10.3847/1538-4357/adb281
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author Yuancheng Xu
Fei Dai
author_facet Yuancheng Xu
Fei Dai
author_sort Yuancheng Xu
collection DOAJ
description Most multiplanet systems around mature (∼5 Gyr old) host stars are nonresonant. Even the near-resonant planet pairs still display 1%–2% positive deviation from perfect period commensurabilities (Δ) near first-order mean motion resonances (MMRs). Resonant repulsion due to eccentricity tides was one of the first mechanisms proposed to explain the observed positive Δ. However, the inferred rates of tidal dissipation are often implausibly rapid (with a reduced tidal quality factor ${Q}_{p}^{{\prime} }\lesssim 10$ ). In this work, we attempt to amplify eccentricity tides with three previously ignored effects. (1) Planets tend to be inflated when they were younger. (2) Kepler-like planets likely form as resonant chains parked at the disk inner edge; overlooked inner planets could have contributed to tidal dissipation of the whole system. (3) Disk migration captures planets into first-order MMR with nonzero initial deviation Δ, thereby lowering the amount of dissipation needed. We show that even after accounting for all three effects, ${Q}_{p}^{{\prime} }$ can only be amplified by about 1 order of magnitude, and still falls short of ${Q}_{p}^{{\prime} }$ values of solar system planets. Therefore, eccentricity tides alone cannot fully explain the observed Δ distribution. Other effects such as obliquity tides, planetesimal scattering, expanding disk inner edge, disk turbulence, divergent encounters, and dynamical instabilities must have contributed to dislodging planets from first-order MMR.
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spelling doaj-art-0e90f68a7c9a45fbb6e2e642305dbb7d2025-08-20T03:15:30ZengIOP PublishingThe Astrophysical Journal1538-43572025-01-01981214210.3847/1538-4357/adb281Amplifying Resonant Repulsion with Inflated Young Planets, Overlooked Inner Planets, and Nonzero Initial ΔYuancheng Xu0Fei Dai1https://orcid.org/0000-0002-8958-0683Department of Physics, Oxford University , Oxford OX1 3RH, UK ; yuancheng.xu@some.ox.ac.ukInstitute for Astronomy, University of Hawai‘i , 2680 Woodlawn Drive, Honolulu, HI 96822, USAMost multiplanet systems around mature (∼5 Gyr old) host stars are nonresonant. Even the near-resonant planet pairs still display 1%–2% positive deviation from perfect period commensurabilities (Δ) near first-order mean motion resonances (MMRs). Resonant repulsion due to eccentricity tides was one of the first mechanisms proposed to explain the observed positive Δ. However, the inferred rates of tidal dissipation are often implausibly rapid (with a reduced tidal quality factor ${Q}_{p}^{{\prime} }\lesssim 10$ ). In this work, we attempt to amplify eccentricity tides with three previously ignored effects. (1) Planets tend to be inflated when they were younger. (2) Kepler-like planets likely form as resonant chains parked at the disk inner edge; overlooked inner planets could have contributed to tidal dissipation of the whole system. (3) Disk migration captures planets into first-order MMR with nonzero initial deviation Δ, thereby lowering the amount of dissipation needed. We show that even after accounting for all three effects, ${Q}_{p}^{{\prime} }$ can only be amplified by about 1 order of magnitude, and still falls short of ${Q}_{p}^{{\prime} }$ values of solar system planets. Therefore, eccentricity tides alone cannot fully explain the observed Δ distribution. Other effects such as obliquity tides, planetesimal scattering, expanding disk inner edge, disk turbulence, divergent encounters, and dynamical instabilities must have contributed to dislodging planets from first-order MMR.https://doi.org/10.3847/1538-4357/adb281Exoplanet astronomyExoplanet tidesExoplanet dynamics
spellingShingle Yuancheng Xu
Fei Dai
Amplifying Resonant Repulsion with Inflated Young Planets, Overlooked Inner Planets, and Nonzero Initial Δ
The Astrophysical Journal
Exoplanet astronomy
Exoplanet tides
Exoplanet dynamics
title Amplifying Resonant Repulsion with Inflated Young Planets, Overlooked Inner Planets, and Nonzero Initial Δ
title_full Amplifying Resonant Repulsion with Inflated Young Planets, Overlooked Inner Planets, and Nonzero Initial Δ
title_fullStr Amplifying Resonant Repulsion with Inflated Young Planets, Overlooked Inner Planets, and Nonzero Initial Δ
title_full_unstemmed Amplifying Resonant Repulsion with Inflated Young Planets, Overlooked Inner Planets, and Nonzero Initial Δ
title_short Amplifying Resonant Repulsion with Inflated Young Planets, Overlooked Inner Planets, and Nonzero Initial Δ
title_sort amplifying resonant repulsion with inflated young planets overlooked inner planets and nonzero initial δ
topic Exoplanet astronomy
Exoplanet tides
Exoplanet dynamics
url https://doi.org/10.3847/1538-4357/adb281
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AT feidai amplifyingresonantrepulsionwithinflatedyoungplanetsoverlookedinnerplanetsandnonzeroinitiald