HATS-38 b and WASP-139 b join a growing group of eccentric hot Neptunes on polar orbits
Juan I. Espinoza-Retamal, Gu{dh}mundur Stef’ansson, Cristobal Petrovich, Rafael Brahm, Andr’es Jord’an, Elyar Sedaghati, Jennifer P. Lucero, Marcelo Tala Pinto, Diego J. Mu~noz, Gavin Boyle, Rodrigo Leiva, Vincent Suc
arXiv:2406.18631v1 Announce Type: new
Abstract: We constrain the sky-projected obliquities of two low-density hot Neptune planets HATS-38 b and WASP-139 b orbiting nearby G and K stars using Rossiter-McLaughlin (RM) observations with VLT/ESPRESSO, yielding $lambda = -108_{-16}^{+11}$ deg and $-85.6_{-4.2}^{+7.7}$ deg, respectively. To model the RM effect, we use a new publicly available code, texttt{ironman}, which is capable of jointly fitting transit photometry, Keplerian radial velocities, and RM effects. The two planets have residual eccentricities ($e= 0.112_{-0.070}^{+0.072}$, and $0.103_{-0.041}^{+0.050}$, respectively), and together with the obliquity constraints, we show that they join a growing group of eccentric hot and low-density Neptunes on polar orbits. We use long-term radial velocities to rule out companions with masses $sim 0.3-50$ $M_J$ within $sim$10 au. We show that the orbital architectures of the two Neptunes disfavor an origin from primordial disk misalignment and/or in-situ secular interactions with distant companions and instead favor high-eccentricity migration from $gtrsim 2$ au driven by a distant companion. Finally, we performed a hierarchical Bayesian modeling of the true obliquity distribution of Neptunes and found suggestive evidence for a higher preponderance of polar orbits of hot Neptunes compared to Jupiters. However, we note that the exact distribution is sensitive to the choice of priors, highlighting the need for additional obliquity measurements of Neptunes to robustly compare the hot Neptune obliquity distribution to Jupiters.arXiv:2406.18631v1 Announce Type: new
Abstract: We constrain the sky-projected obliquities of two low-density hot Neptune planets HATS-38 b and WASP-139 b orbiting nearby G and K stars using Rossiter-McLaughlin (RM) observations with VLT/ESPRESSO, yielding $lambda = -108_{-16}^{+11}$ deg and $-85.6_{-4.2}^{+7.7}$ deg, respectively. To model the RM effect, we use a new publicly available code, texttt{ironman}, which is capable of jointly fitting transit photometry, Keplerian radial velocities, and RM effects. The two planets have residual eccentricities ($e= 0.112_{-0.070}^{+0.072}$, and $0.103_{-0.041}^{+0.050}$, respectively), and together with the obliquity constraints, we show that they join a growing group of eccentric hot and low-density Neptunes on polar orbits. We use long-term radial velocities to rule out companions with masses $sim 0.3-50$ $M_J$ within $sim$10 au. We show that the orbital architectures of the two Neptunes disfavor an origin from primordial disk misalignment and/or in-situ secular interactions with distant companions and instead favor high-eccentricity migration from $gtrsim 2$ au driven by a distant companion. Finally, we performed a hierarchical Bayesian modeling of the true obliquity distribution of Neptunes and found suggestive evidence for a higher preponderance of polar orbits of hot Neptunes compared to Jupiters. However, we note that the exact distribution is sensitive to the choice of priors, highlighting the need for additional obliquity measurements of Neptunes to robustly compare the hot Neptune obliquity distribution to Jupiters.

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