Bibcode
Bonfanti, A.; Amateis, I.; Gandolfi, D.; Borsato, L.; Egger, J. A.; Cubillos, P. E.; Armstrong, D.; Leão, I. C.; Fridlund, M.; Canto Martins, B. L.; Sousa, S. G.; De Medeiros, J. R.; Fossati, L.; Adibekyan, V.; Collier Cameron, A.; Grziwa, S.; Lam, K. W. F.; Goffo, E.; Nielsen, L. D.; Rodler, F.; Alarcon, J.; Lillo-Box, J.; Cochran, W. D.; Luque, R.; Redfield, S.; Santos, N. C.; Barros, S. C. C.; Bayliss, D.; Dumusque, X.; Keniger, M. A. F.; Livingston, J.; Murgas, F.; Nowak, G.; Osborn, A.; Osborn, H. P.; Pallé, E.; Persson, C. M.; Serrano, L. M.; Strøm, P. A.; Udry, S.; Wheatley, P. J.
Bibliographical reference
Astronomy and Astrophysics
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1
2025
Journal
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0
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Description
Context. TOI-396 is an F6 V bright naked-eye star (V ≈ 6.4) orbited by three small (Rp ≈ 2 R⊕) transiting planets discovered thanks to space-based photometry from two TESS sectors. The orbital periods of the two innermost planets, namely TOI-396 b and c, are close to the 5:3 commensurability (Pb ~ 3.6 d and Pc ~ 6.0 d), suggesting that the planets might be trapped in a mean motion resonance (MMR). Aims. To measure the masses of the three planets, refine their radii, and investigate whether planets b and c are in MMR, we carried out HARPS radial velocity (RV) observations of TOI-396 and retrieved archival high-precision transit photometry from four TESS sectors. Methods. We extracted the RVs via a skew-normal fit onto the HARPS cross-correlation functions and performed a Markov chain Monte Carlo joint analysis of the Doppler measurements and transit photometry, while employing the breakpoint method to remove stellar activity from the RV time series. We also performed a transit timing variation (TTV) dynamical analysis of the system and simulated the temporal evolution of the TTV amplitudes of the three planets following an N-body numerical integration. Results. Our analysis confirms that the three planets have similar sizes (Rb = 2.004‑0.047+0.045 R⊕ ; Rc = 1.979‑0.051+0.054 R⊕; Rd = 2.001‑0.064+0.063 R⊕) and is thus in agreement with previous findings. However, our measurements are ~ 1.4 times more precise thanks to the use of two additional TESS sectors. For the first time, we have determined the RV masses for TOI-396 b and d, finding them to be Mb = 3.55‑0.96+0.94 M⊕ and Md = 7.1 ± 1.6 M⊕, which implies bulk densities of ρb = 2.44‑0.68+0.69 g cm‑3 and ρd = 4.9‑1.1+1.2 g cm‑3, respectively. Our results suggest a quite unusual system architecture, with the outermost planet being the densest. Based on a frequency analysis of the HARPS activity indicators and TESS light curves, we find the rotation period of the star to be Prot,⋆ = 6.7 ± 1.3 d, in agreement with the value predicted from log R'HK-based empirical relations. The Doppler reflex motion induced by TOI-396 c remains undetected in our RV time series, likely due to the proximity of the planet's orbital period to the star's rotation period. We also discovered that TOI-396 b and c display significant TTVs. While the TTV dynamical analysis returns a formally precise mass for TOI-396 c of Mc,dyn = 2.24‑0.67+0.13 M⊕, the result might not be accurate, owing to the poor sampling of the TTV phase. We also conclude that TOI-396 b and c are close to but out of the 5:3 MMR. Conclusions. A TTV dynamical analysis of additional transit photometry evenly covering the TTV phase and super-period is likely the most effective approach for precisely and accurately determining the mass of TOI-396 c. Our numerical simulation suggests TTV semi-amplitudes of up to five hours over a temporal baseline of ~ 5.2 years, which should be duly taken into account when scheduling future observations of TOI-396. ★Based on observations performed with the 3.6 m telescope at the European Southern Observatory (La Silla, Chile) under programmes 1102.C-0923, 1102.C-0249, 0102.C-0584, and 60.A-9700.