2019
DOI: 10.1093/mnras/stz535
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3D simulations of planet trapping at disc–cavity boundaries

Abstract: Inward migration of low-mass planets and embryos of giant planets can be stopped at the disc-cavity boundaries due to co-orbital corotation torque. We performed the first global three-dimensional (3D) simulations of planet migration at the disc-cavity boundary, and have shown that the boundary is a robust trap for low-mass planets and embryos. A protoplanetary disc may have several such trapping regions at various distances from the star, such as at the edge of the stellar magnetosphere, the inner edge of the … Show more

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Cited by 34 publications
(31 citation statements)
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“…The radius at which this occurs is often called a planet trap, since the torque balance will cause a planet to halt migration and become trapped at a fixed orbital radius. This behavior has been found in several other numerical studies (e.g., Morbidelli et al 2008;Baillié et al 2016;Romanova et al 2019). Since the planets we consider in this work reside at (or near) the inner disk edge, slightly external to the interior cavity, Type I torques are expected to act outward, and under standard assumptions, C I ≈ −0.6 (Ward 1997;Tanaka et al 2002).…”
Section: Type I Torquessupporting
confidence: 78%
“…The radius at which this occurs is often called a planet trap, since the torque balance will cause a planet to halt migration and become trapped at a fixed orbital radius. This behavior has been found in several other numerical studies (e.g., Morbidelli et al 2008;Baillié et al 2016;Romanova et al 2019). Since the planets we consider in this work reside at (or near) the inner disk edge, slightly external to the interior cavity, Type I torques are expected to act outward, and under standard assumptions, C I ≈ −0.6 (Ward 1997;Tanaka et al 2002).…”
Section: Type I Torquessupporting
confidence: 78%
“…Migrating cores tend to form configurations in which each pair of neighboring planets is in mean motion resonance (e.g., Cresswell & Nelson, 2008;Terquem & Papaloizou, 2007). In these "resonant chains," the innermost planet is anchored at the inner edge of the gaseous disk, which provides a positive torque to balance the negative ones felt by the other planets (Masset et al, 2006;Romanova et al, 2019). Resonant chains often become dynamically unstable after the gaseous disk dissipates, leading to phase of late giant impacts (Cossou et al, 2014;Ogihara & Ida, 2009;Terquem & Papaloizou, 2007).…”
Section: Silicate Water Ironmentioning
confidence: 99%
“…where f " exp r´pr p´rin q{x hs s is a smooth fitting function, r p is the planet disk location, and f "1 (f "0) refers to the planet at the disk edge (far away from the disk edge). Although the above equations are derived analytically, we note that the termination of planet migration at the inner disk edge due to one-sided torque induced from a steep density transition is also obtained from hydrodynamic simulations 25,26 .…”
Section: Methodsmentioning
confidence: 99%
“…In contrast, planets at the disk's inner edge only interact with gas on the outside of their orbits. As a result of larger-amplitude Lindblad and corotation torques, a planet below the mass threshold for opening a gap stops migrating inward at the disk inner edge 25,26 . If the disk inner edge is itself moving radially outward due to disk dispersal, then the planet may subsequently migrate outward along with the expanding inner edge (see Supplementary Information).…”
mentioning
confidence: 99%