J/A+A/709/A60       Wave breaking predictions for hot Jupiters (Golonka+, 2026)

Planet-star interactions with precise transit timing. V. Tidal decay of hot Jupiters through wave breaking. Golonka J., Maciejewski G. <Astron. Astrophys. 709, A60 (2026)> =2026A&A...709A..60G 2026A&A...709A..60G (SIMBAD/NED BibCode)
ADC_Keywords: Stars, double and multiple ; Exoplanets ; Binaries, orbits ; Optical Keywords: planet-star interactions Abstract: Tidal interactions shape the evolution of close-in giant planets, and internal-gravity-wave breaking offers an efficient pathway for dynamical-tide dissipation, though its population-wide impact remains poorly constrained. We aim to quantify wave-breaking tidal dissipation for 550 hot Jupiters, accounting for stellar-parameter uncertainties, and to identify the most promising systems for detecting orbital decay through transit timing. Stellar masses, radii, and ages were homogeneously redetermined from spectroscopic and photometric data using isochrone fitting. For each system, these parameters were propagated through a dedicated MESA model grid to calculate the tidal quality factor, wave-breaking probability, orbital decay rate, and transit- timing diagnostics. Long-term orbital evolution was modelled to predict planetary destruction timescales. Wave breaking is predicted to be largely inactive in pre-intermediate-age main sequence (IAMS) stars. For hosts with masses <1.2M☉, it becomes effective after the IAMS, while in more massive stars it begins between the IAMS and the terminal-age main sequence (TAMS). The tidal quality factor for systems undergoing wave breaking peaks between 10^6 and 10^7, consistent with population-level inferences. About 43 % of planets, mostly with periods <3.5d, are expected to inspiral on the main sequence, providing a physical explanation for the observed tendency of hot Jupiters to orbit younger stars. A further 41 % inspiral during post-main- sequence evolution within the stages considered. Roche-limit disruption dominates overall, with engulfment occurring mainly for planets with periods > 5-6d. Systems with periods <1d, that could in principle experience the strongest tidal forcing, are unlikely to trigger wave breaking, leaving planets on stable orbits. Conversely, the most rapidly inspiralling systems with high wave-breaking probability may display measurable orbital-period shortening only over multi-decade baselines, eluding immediate detection. By contrast, the demographic imprint of wave breaking on occurrence rates should emerge more readily, with the first signs already visible in current population statistics. Description: The full dataset used to study wave breaking for the 550 hot Jupiter systems. The additional WASP 12 subgiant scenario is also available in the data as 'WASP-12 Ab subgiant'. The general and spectroscopic parameters, the results from the isochrones fit and wave breaking predictions for each system are presented in tables 1, 2 and 3 respectively. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tablea1.dat 250 551 Spectroscopic and general parameters of the studied systems tablea2.dat 428 551 Results of the isochrones fits tablea3.dat 537 551 Wave breaking predictions -------------------------------------------------------------------------------- See also: J/AcA/68/371 : WASP and KELT planet transits (Maciejewski+, 2018) J/AcA/70/1 : WASP-18 Photometric timeseries and timing data (Maciejewski+, 2020) J/A+A/667/A127 : Photometric timeseries and transit times (Maciejewski+, 2022) https://sweetcat.iastro.pt : SWEET-cat Home Page Byte-by-byte Description of file: tablea1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 19 A19 --- Name Planet name 21- 33 F13.11 d Porb Orbital period 35- 42 F8.2 m/s K ? Radial velocity amplitude 44- 50 F7.3 deg i ? Inclination of the orbit 52- 70 F19.16 Mjup Mp Planets mass 72- 88 F17.14 --- aR Semimajor axis in host radii 90- 99 F10.8 --- rprs Planet to star radius ratio 101-104 I4 "date" Disc Discovery year 106-109 I4 K Teffl Effective temperature of the host from literature 111-113 I3 K e_Teffl Uncertainty of effective temperature of the host from literature 115-119 F5.3 --- loggl Logarithm of stellar gravity from literature 121-125 F5.3 --- e_loggl Uncertainty of stellar gravity from literature 127-132 F6.3 --- [Fe/H]l Metallicity from literature 134-138 F5.3 --- e_[Fe/H]l Uncertainty of metallicity from literature 140-146 F7.4 mas Plx Gaia parallax 148-166 F19.17 mas e_Plx Uncertainty of Gaia parallax 168-176 F9.6 mag Gmag Magnitude in Gaia G filter 178-185 F8.6 mag e_Gmag Uncertainty of magnitude in Gaia G filter 187-195 F9.6 mag RPmag Magnitude in Gaia RP filter 197-204 F8.6 mag e_RPmag Uncertainty of magnitude in Gaia RP filter 206-214 F9.6 mag BPmag Magnitude in Gaia BP filter 216-223 F8.6 mag e_BPmag Uncertainty of magnitude in Gaia BP filter 225-250 A26 --- Source Literature source of spectroscopic data from SWEETCAT, https://sweetcat.iastro.pt -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablea2.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 19 A19 --- Name Planet name 21- 37 F17.14 [yr] logAge Logarithm of the age of the host star 39- 58 F20.18 [yr] e_logAge Lower uncertainty of logarithm of the age of the host star 60- 79 F20.18 [yr] E_logAge Upper uncertainty of logarithm of the age of the host star 81- 97 F17.15 Msun Mass Mass of the host star 99-118 F20.18 Msun e_Mass Lower uncertainty of mass of the host star 120-138 F19.17 Msun E_Mass Upper uncertainty of mass of the host star 140-156 F17.15 Rsun R Radius of the host star 158-177 F20.18 Rsun e_R Lower uncertainty of radius of the host star 179-197 F19.17 Rsun E_R Upper uncertainty of radius of the host star 199-219 F21.18 --- [Fe/H] Metallicity 221-239 F19.17 --- e_[Fe/H] Lower uncertainty of metallicity 241-259 F19.17 --- E_[Fe/H] Upper uncertainty of metallicity 261-276 F16.11 K Teff Effective temperature of the host 278-295 F18.14 K e_Teff Lower uncertainty of effective temperature of the host 297-314 F18.14 K E_Teff Upper uncertainty of effective temperature of the host 316-331 F16.14 [cm/s2] logg Stellar gravity 333-351 F19.17 [cm/s2] e_logg Lower uncertainty of stellar gravity 353-372 F20.18 [cm/s2] E_logg Upper uncertainty of stellar gravity 374-389 F16.12 --- eep Equivalent evolutionary point 391-409 F19.16 --- e_eep Lower uncertainty of equivalent evolutionary point 411-428 F18.15 --- E_eep Upper uncertainty of equivalent evolutionary point -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablea3.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 19 A19 --- Name Planet name 21- 22 I2 --- Nout Number of realisations out of 100 that fell outside of the MESA grid 24- 76 A53 --- Notes Notes about predictions 78-103 F26.10 --- Q ? Reduced tidal quality factor 105-132 F28.12 --- e_Q ? Lower uncertainty of reduced tidal quality factor 134-160 F27.12 --- E_Q ? Upper uncertainty of reduced tidal quality factor 162-179 F18.14 --- Mcrit Probability of wave breaking 181-211 E31.22 s Tshift2025 ? Shift in central transit times by 2025 213-239 E27.21 s e_Tshift2025 ? Lower uncertainty of shift in central transit times by 2025 241-267 E27.21 s E_Tshift2025 ? Upper uncertainty of shift in central transit times by 2025 269-288 F20.11 yr Tshift5min ? Predicted year when the cumulative shift reaches 5 minutes 290-313 F24.16 yr e_Tshift5min ? Lower uncertainty of predicted year when the cumulative shift reaches 5 minutes 315-337 F23.15 yr E_Tshift5min ? Upper uncertainty of predicted year when the cumulative shift reaches 5 minutes 339-364 E26.20 ms/yr Pdot ? Orbital period change 366-390 E25.19 ms/yr e_Pdot ? Lower uncertainty of orbital period change 393-418 E26.20 ms/yr E_Pdot ? Upper uncertainty of orbital period change 420-436 F17.14 [yr] logAgedest ? Logarithm of the age of destruction 438-458 F21.18 [yr] e_logAgedest ? Lower uncertainty of logarithm of the age of destruction 460-479 F20.17 [yr] E_logAgedest ? Upper uncertainty of logarithm of the age of destruction 481-497 F17.12 --- eepdest ? Equivalent evolutionary point of destruction 499-517 F19.15 --- e_eepdest ? Lower uncertainty of equivalent evolutionary point of destruction 519-537 F19.15 --- E_eepdest ? Upper uncertainty of equivalent evolutionary point of destruction -------------------------------------------------------------------------------- Acknowledgements: Jan Golonka, jgolonka(at)doktorant.umk.pl Institute of Astronomy, Nicolaus Copernicus Univeristy, Poland References: Maciejewski et al., Paper I 2018AcA....68..371M 2018AcA....68..371M, Cat. J/AcA/68/371 Maciejewski et al., Paper II 2020AcA....70....1M 2020AcA....70....1M, Cat. J/AcA/70/1 Maciejewski et al., Paper III 2022A&A...667A.127M 2022A&A...667A.127M, Cat. J/A+A/667/A127 Maciejewski et al., Paper IV 2024A&A...692A..35M 2024A&A...692A..35M, Cat. J/A+A/692/A35 Sousa et al., 2021A&A...656A..53S 2021A&A...656A..53S, SWEET-Cat 2.0: The Cat just got SWEETer https://sweetcat.iastro.pt Barker et al., 2020MNRAS.498.2270B 2020MNRAS.498.2270B, Tidal dissipation in evolving low-mass and solar-type stars with predictions for planetary orbital decay License: CC-BY-4.0
(End) Jan Golonka [Copernicus Univ.], Patricia Vannier [CDS] 08-Apr-2026
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