The tidal deformation and atmosphere of WASP-12b from its phase curve
Abstract
Ultra-hot Jupiters present a unique opportunity to understand the physics and chemistry of planets at extreme conditions. WASP-12b stands out as an archetype of this class of exoplanets. We performed comprehensive analyses of the transits, occultations, and phase curves of WASP-12b by combining new CHEOPS observations with previous TESS and Spitzer data to measure the planet's tidal deformation, atmospheric properties, and orbital decay rate. The planet was modeled as a triaxial ellipsoid parameterized by the second-order fluid Love number, , which quantifies its radial deformation and provides insight into the interior structure. We measured the tidal deformation of WASP-12b and estimated a Love number of (at 3.2) from its phase curve. We measured occultation depths of ppm and ppm in the CHEOPS and TESS bands, respectively, while the dayside emission spectrum indicates that CHEOPS and TESS probe similar pressure levels in the atmosphere at a temperature of 2900K. We also estimated low geometric albedos of and in the CHEOPS and TESS passbands, respectively, suggesting the absence of reflective clouds in the dayside of the WASP-12b. The CHEOPS occultations do not show strong evidence for variability in the dayside atmosphere of the planet. Finally, we refine the orbital decay rate by 12% to a value of -30.230.82 ms/yr. WASP-12b becomes the second exoplanet, after WASP-103b, for which the Love number has been measured (at 3) from the effect of tidal deformation in the light curve. However, constraining the core mass fraction of the planet requires measuring with a higher precision. This can be achieved with high signal-to-noise observations with JWST since the phase curve amplitude, and consequently the induced tidal deformation effect, is higher in the infrared.
Cite
@article{arxiv.2402.10486,
title = {The tidal deformation and atmosphere of WASP-12b from its phase curve},
author = {B. Akinsanmi and S. C. C. Barros and M. Lendl and L. Carone and P. E. Cubillos and A. Bekkelien and A. Fortier and H. -G. Florén and A. Collier Cameron and G. Boué and G. Bruno and B. -O. Demory and A. Brandeker and S. G. Sousa and T. G. Wilson and A. Deline and A. Bonfanti and G. Scandariato and M. J. Hooton and A. C. M. Correia and O. D. S. Demangeon and A. M. S. Smith and V. Singh and Y. Alibert and R. Alonso and J. Asquier and T. Bárczy and D. Barrado Navascues and W. Baumjohann and M. Beck and T. Beck and W. Benz and N. Billot and X. Bonfils and L. Borsato and Ch. Broeg and M. Buder and S. Charnoz and Sz. Csizmadia and M. B. Davies and M. Deleuil and L. Delrez and D. Ehrenreich and A. Erikson and J. Farinato and L. Fossati and M. Fridlund and D. Gandolfi and M. Gillon and M. Güdel and M. N. Günther and A. Heitzmann and Ch. Helling and S. Hoyer and K. G. Isaak and L. L. Kiss and K. W. F. Lam and J. Laskar and A. Lecavelier des Etangs and D. Magrin and P. F. L. Maxted and M. Mecina and Ch. Mordasini and V. Nascimbeni and G. Olofsson and R. Ottensamer and I. Pagano and E. Pallé and G. Peter and D. Piazza and G. Piotto and D. Pollacco and D. Queloz and R. Ragazzoni and N. Rando and H. Rauer and I. Ribas and N. C. Santos and D. Ségransan and A. E. Simon and M. Stalport and Gy. M. Szabó and N. Thomas and S. Udry and V. Van Grootel and J. Venturini and E. Villaver and N. A. Walton},
journal= {arXiv preprint arXiv:2402.10486},
year = {2024}
}
Comments
accepted for publication in A&A