2010
DOI: 10.1088/0004-637x/721/2/1184
|View full text |Cite
|
Sign up to set email alerts
|

Eccentricity Trap: Trapping of Resonantly Interacting Planets Near the Disk Inner Edge

Abstract: Using orbital integration and analytical arguments, we have found a new mechanism (an "eccentricity trap") to halt type I migration of planets near the inner edge of a protoplanetary disk. Because asymmetric eccentricity damping due to disk-planet interaction on the innermost planet at the disk edge plays a crucial role in the trap, this mechanism requires continuous eccentricity excitation and hence works for a resonantly interacting convoy of planets. This trap is so strong that the edge torque exerted on th… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
66
1

Year Published

2010
2010
2016
2016

Publication Types

Select...
8
1

Relationship

4
5

Authors

Journals

citations
Cited by 64 publications
(67 citation statements)
references
References 24 publications
(49 reference statements)
0
66
1
Order By: Relevance
“…2, the former can become positive owing to the corotation torque, which depends on the slope of the gas surface density. The latter is a torque recently found by Ogihara et al (2010). When a body with non-zero eccentricity straddles a sharp disk inner edge, the body gains a net positive torque from the disk depending on the sharpness of the edge and on the eccentricity.…”
Section: Orbital Evolutionmentioning
confidence: 72%
“…2, the former can become positive owing to the corotation torque, which depends on the slope of the gas surface density. The latter is a torque recently found by Ogihara et al (2010). When a body with non-zero eccentricity straddles a sharp disk inner edge, the body gains a net positive torque from the disk depending on the sharpness of the edge and on the eccentricity.…”
Section: Orbital Evolutionmentioning
confidence: 72%
“…In the case of a smooth density profile (q ≈ 0), explicit expressions for the forces acting on the planetary masses can be found in Ogihara & Ida (2009) and Ogihara et al (2010), while the applications of the model can be found in Giuppone et al (2012). In our simulation, we assume a scale height h = H/r = 0.05 and a constant surface density profile Σ(r) = Σ 0 (r/1 AU) −q with q = 0 and Σ 0 = 300 g/cm 2 , which corresponds to two minimum mass solar nebula at 5 AU (MMSN, Hayashi 1981).…”
Section: Hd 200964 Star Mass Evaluationmentioning
confidence: 99%
“…It is worth mentioning that the model is valid only for low eccentricities (e < ∼ 0.05) and small planetary masses ( < ∼ 13 M ⊕ ). In the case of a smooth density profile, explicit expressions for the forces acting on the planetary masses can be found in Ogihara & Ida (2009) and Ogihara et al (2010), while model applications can be found in Giuppone et al (2012). In our simulation, we assumed a scale height h = H/r = 0.05 and a constant surface density profile Σ(r) = Σ 0 (r/1 AU) −q with q = 0 and Σ 0 = 150 g/cm 2 , which corresponds to the minimum mass solar nebula at 5 AU (MMSN, Hayashi 1981).…”
Section: Scenario 2 For the Origin Of The 3/2 Resonance For The Hd 45mentioning
confidence: 99%