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Cloutier, R; Charbonneau, D; Stassun, K G; Murgas, F; Mortier, A; Massey, R; Lissauer, J J; Latham, D W; Irwin, J; Haywood, R D; Guerra, P; Girardin, E; Giacalone, S A; Bosch-Cabot, P; Bieryla, A; Winn, J; Watson, C A; Vanderspek, R; Udry, S; Tamura, M; Sozzetti, A; Shporer, A; Ségransan, D; Seager, S; Savel, A B; Sasselov, D; Rose, M; Ricker, G; Rice, K; Quintana, E V; Quinn, S N; Piotto, G; Phillips, D; Pepe, F; Pedani, M; Parviainen, H; Palle, E; Narita, N; Molinari, E; Micela, G; McDermott, S; Mayor, M; Matson, R A; Martinez Fiorenzano, A F; Lovis, C; López-Morales, M; Kusakabe, N; Jensen, E L N; Jenkins, J M; Huang, C X; Howell, S B; Harutyunyan, A; Fűrész, G; Fukui, A; Esquerdo, G A; Esparza-Borges, E; Dumusque, X; Dressing, C D; L Di Fabrizio; Collins, K A; A Collier Cameron; Christiansen, J L; Cecconi, M; Buchhave, L A; Boschin, W; Andreuzzi, G
arXiv.org, 05/2021Paper, Journal Article
Studies of close-in planets orbiting M dwarfs have suggested that the M dwarf radius valley may be well-explained by distinct formation timescales between enveloped terrestrials, and rocky planets that form at late times in a gas-depleted environment. This scenario is at odds with the picture that close-in rocky planets form with a primordial gaseous envelope that is subsequently stripped away by some thermally-driven mass loss process. These two physical scenarios make unique predictions of the rocky/enveloped transition's dependence on orbital separation such that studying the compositions of planets within the M dwarf radius valley may be able to establish the dominant physics. Here, we present the discovery of one such keystone planet: the ultra-short period planet TOI-1634 b (\(P=0.989\) days, \(F=121 F_{\oplus}\), \(r_p = 1.790^{+0.080}_{-0.081} R_{\oplus}\)) orbiting a nearby M2 dwarf (\(K_s=8.7\), \(R_s=0.45 R_{\odot}\), \(M_s=0.50 M_{\odot}\)) and whose size and orbital period sit within the M dwarf radius valley. We confirm the TESS-discovered planet candidate using extensive ground-based follow-up campaigns, including a set of 32 precise radial velocity measurements from HARPS-N. We measure a planetary mass of \(4.91^{+0.68}_{-0.70} M_{\oplus}\), which makes TOI-1634 b inconsistent with an Earth-like composition at \(5.9\sigma\) and thus requires either an extended gaseous envelope, a large volatile-rich layer, or a rocky portion that is not dominated by iron and silicates to explain its mass and radius. The discovery that the bulk composition of TOI-1634 b is inconsistent with that of the Earth favors the gas-depleted formation mechanism to explain the emergence of the radius valley around M dwarfs with \(M_s\lesssim 0.5 M_{\odot}\).
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