on the origin of the long-lived asteroids in the 2:1 mean-motion...
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On the Origin of the Long-Lived Asteroidsin the 2:1 Mean-Motion Resonance
with Jupiter
O. Chrenko1, M. Broz1, D. Nesvorny2
1 Astronomical Institute, Faculty of Mathematics and Physics,Charles University in Prague
2 Southwest Research Institute, Boulder, Colorado
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e
a [AU]
2:1
Data in figure by Knezevic & Milani (2003)
Motivation and update
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reso
nant
ecc
entr
icity
er
resonant semi-major axis ar [AU]
island A
island B
Kozai
ν16
ν5
2/1 separatrix 0
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reso
nant
incl
inat
ion
sin
I r
resonant semi-major axis ar [AU]
stable B:I < 5°
stable A:I > 5°
124 dynamically stable asteroids (lifetime > 1Gyr) and106 marginally stable asteroids (0.07Gyr < lifetime ≤ 1Gyr)
◮ resonant elements computed according to Roig et al. (2002)◮ primordial origin or resonant capture? the presentation is
focused on the latter
(some) previous papers on the origin: Moons et al. (1998), Ferraz-Mello et al. (1998),Roig et al. (2002), Broz et al. (2005), Broz & Vokrouhlicky (2008) 2 / 8
Migration scenarios and methods
◮ orbital evolution of planets prescribed according to scenariosby Nesvorny & Morbidelli (2013), Morbidelli et al. (2010)
fifth giant planet scenariojumping Jupiter scenario with four giant planets
◮ planets: interpolation in cartesian coordinates (x , y , z) alongKeplerian ellipses; input data sampling ∆t = 1 yr
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a, q
, Q [A
U]
time t [Myr]
Jupiter
Saturn
Uranus
Neptune
5th planet
◮ test particles: symplectic SWIFT-RMVS algorithm(Levison & Duncan 1994) with 0.25 yr timestep
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Capture in the fifth-giant-planet scenario
◮ initial population of 5000 test particles with isotropic (a, e, I )distribution in the outer main belt; I ∈ (0◦, 15◦)
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0.5migrating
2:1 center
t = 2 Myr
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nant
ecc
entr
icity
er
resonant semi-major axis ar [AU]
t = 6.26 MyrJump!
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t = 10 Myr
◮ capture is significant, but which asteroids are long-lived?4 / 8
Dynamical map present configuration of planets
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city
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resonant semi-major axis ar [AU]
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dist
ance
d
ν16
ν5
Kozai
island A
island B
secondaryresonances
separatrix
◮ δ ≡ the difference between the initial and final resonantelement over 10 Myr timespan
◮ distance d ≡
√
(
δarar
)2+ (δer)
2 + (δ sin Ir)2
◮ 24000 test particles per simulation5 / 8
Dynamical map post-migration configuration of planets
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city
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resonant semi-major axis ar [AU]
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ance
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◮ the post-migration map is used to extract the long-livedasteroids at the end of our simulations(i.e. similar structure, stable islands exist)
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Result: Captured long-lived asteroids
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city
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resonant semi-major axis ar [AU]
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dist
ance
d
◮ initial population rescaled to outer main belt values– captured population increased by factor 10 to 13
◮ long-term depletion rate applied– 93% to 95% decay over 4 Gyr; by Skoulidou et al. (CPS-IAU, 2014)
◮ 158 to 219 test particles in B (vs 180 observed) - match◮ 37 to 51 test particles in A (vs 11 observed) - mismatch
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Conclusions (and confusions)
◮ capture works in the fifth-giant-planet scenario with1.5% efficiency in the island A and with 5% efficiency in B
◮ moreover, 3% of the primordial population survives the jump!
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icity
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resonant semi-major axis ar [AU]
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dist
ance
d
◮ how to explain the observed steep SFD (cumulative slope −4.3)?
◮ is primordial population really primordial?
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