Academia Sinica Institute of Astronomy and Astrophysics, Department of Physics, National University of Taiwan Dec 2, 2014
69 slides
Ubiquity of planets and diversity of planetary systems:
Origin and Destiny of multiple super Earths and gas giants.
Douglas N.C. Lin
Astronomy (UCSC), KIAA (PKU), IAS (THU)
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The unknown unknowns
Search for extra terrestrial intelligence (SETI)
3/69 Drake Equation
Radial velocity
Femtometer Doppler shift In individual lines
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Precision COSMOGONY
• Ubiquity of planets:
case study vs Science
• Diversity of systems:
realm of possibilities
• Population census
missing info & big picture
• Solar system connection Anthropic principle
Integral of details
Survival of fittest
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Transit (eclipse) searches
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Transit of Venus
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Conventional core accretion scenario
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Major Challenges:
• Retention of grains: m-size barrier (Whipple)
• Fragmentation: km-size barrier (Benz)
• Planetesimal-growth barrier: Isolation mass barrier (Wetherill)
• Gas accretion barrier: critical-mass cores (Cameron)
• Retention of cores: type I migration (Goldreich &
Tremaine, Ward)
• Retention of gas giants: type II migration (Lin &
Papaloizou)
• Multiple gas giants: rapid depletion of disk gas
• Competing physics on multiple length & time scales
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Step I: Meter-barrier Hydrodynamic drag on dusts
Zhang Yuan 12/69
Trapping locations: transition fronts and wall of magnetospheric cavity
9/59 Lecar asteroid 4417 13/69
Major Challenges:
• Retention of grains: m-size barrier (Whipple)
• Fragmentation: km-size barrier (Benz)
• Planetesimal-growth barrier: Isolation mass barrier (Wetherill)
• Gas accretion barrier: critical-mass cores (Cameron)
• Retention of cores: type I migration (Goldreich &
Tremaine, Ward)
• Retention of gas giants: type II migration (Lin &
Papaloizou)
• Multiple gas giants: rapid depletion of disk gas
• Competing physics on multiple length & time scales
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Planetesimal growth in a trap
Rixin Li, Yuan Zhang, Bili Dong
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Stalling of planets inside & at the magnetospheric truncation radius
Hartmann et al. 1998
Mass Accretion Rate Stellar Dipole Moment
16/69 Magnetosphere radius
Herczeg
Major Challenges:
• Retention of grains: m-size barrier (Whipple)
• Fragmentation: km-size barrier (Benz)
• Planetesimal-growth barrier: Isolation mass barrier (Wetherill)
• Gas accretion barrier: critical-mass cores (Cameron)
• Retention of embryos: type I migration (Goldreich &
Tremaine, Ward)
• Retention of gas giants: type II migration (Lin &
Papaloizou)
• Multiple gas giants: rapid depletion of disk gas
• Competing physics on multiple length & time scales
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Step III, oligarchic barrier: Isolation mass
Feeding zones: D ~ 10 r
HillIsolation mass: M
isolation~ S
1.5a
3M
*-1/2Kokubo & Ida
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Major Challenges:
• Retention of grains: m-size barrier (Whipple)
• Fragmentation: km-size barrier (Benz)
• Planetesimal-growth barrier: Isolation mass barrier (Wetherill)
• Proliferation of multiple, wide spread embryos
• Diversity of planetary architecture
• Retention of gas giants: type II migration (Lin &
Papaloizou)
• Multiple gas giants: rapid depletion of disk gas
• Competing physics on multiple length & time scales
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The planet exchanges angular momentum with:
- circulating fluid elements:
- librating fluid elements:
Maximum value scales with - gradient of disk vortensity (Ω/2Σ) across horseshoe region
Step IV, Embryos barrier: planetary migration Type I migration of super-Earth in isothermal disks
→ corotation torque
e.g. Goldreich & Tremaine (1980), Ward (1992) Masset (2001), Paadekooper, Baruteau, Kley
α = 0 α = 5x10-5
α = 10-2
Long-term evolution of the corotation torque is related to the disk viscosity Paardekooper, Baruteau,
→ differential Lindblad torque
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Planet-disk tidal interaction
Total tidal torque:
= f(p,q,p
n,q
n, p
k, q
k) G
0p and q depend on disk structure &
p
n,q
n,p
k, and q
kalso depend on m
p(1/e)de/dt = (a/H)
4(M
pSa
2/M
*2) W
21/69 Lecar et al, Garaud, Kretke22/69
Resonant sweeping of planetesimals
Major Challenges:
• Retention of grains: m-size barrier (Whipple)
• Fragmentation: km-size barrier (Benz)
• Planetesimal-growth barrier: Isolation mass barrier (Wetherill)
• Gas accretion barrier: critical-mass cores (Cameron)
• Retention of embryos: type I migration (Goldreich &
Tremaine, Ward)
• Retention of gas giants: type II migration (Lin &
Papaloizou)
• Multiple gas giants: rapid depletion of disk gas
• Competing physics on multiple length & time scales
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Core barrier: embryos’ resonant trapping
24/69 M=1Msun, Mdot = 10-8M_sun/yr, a=10-3
Beibei Liu
Loss of massive super-Earth embryos?
No shortage of building block materials
Major Challenges:
• Retention of grains: m-size barrier (Whipple)
• Fragmentation: km-size barrier (Benz)
• Planetesimal-growth barrier: Isolation mass barrier (Wetherill)
• Gas accretion barrier: critical-mass cores (Cameron)
• Retention of cores: type I migration (Goldreich &
Tremaine, Ward)
• Retention of gas giants: type II migration (Lin &
Papaloizou)
• Multiple gas giants: rapid depletion of disk gas
• Competing physics on multiple length & time scales
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Radiation transfer & gas accretion
• Is there a threshold mass for gas accretion? Gas accretion barrier:
Klahr Pollack et al
Ikoma
Bypass the resonance barrier
Orbit crossing, close encounters, home coming & collisions 27/69
Giant impacts of super Earths
Liu Shangfei 28/69
Major Challenges:
• Retention of grains: m-size barrier (Whipple)
• Fragmentation: km-size barrier (Benz)
• Planetesimal-growth barrier: Isolation mass barrier (Wetherill)
• Availability of building block material
• Frequency of planets around different type stars
• Retention of gas giants: type II migration (Lin &
Papaloizou)
• Multiple gas giants: rapid depletion of disk gas
• Competing physics on multiple length & time scales
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Dependence on stellar mass
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Dependence on the disks’ accretion rate
Mdot = 10-8 5 x10-8 10-7
2Msun
1Msun
0.5Msun
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Dependence on the disks’ accretion rate
1) Cores’ migration speed is determined by the surface density of the disk gas.
2) Surface density of the disk gas
is proportional to the gas accretion rate 3) Gas accretion is observed to increase with the host stars’ mass.
4) Gas giants’ frequency correlation with the host stars’ mass is through mdot.
Cores enter orbit crossing zone 0.5Mo
2Mo
Resonant barrier
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Planetary mass & size vs stellar metallicity
There is a strong correlation between h
HJvs stellar metallicity.
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Abundance of super Earths
There is no shortage of super Earths around metal-poor stars
Formation of super Earths Does not depend on Z or M
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Dependence on metallicity
Fe/H=1 Fe/H=3
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Migration in metal-rich disks
Fe/H=1/3
Fe/H=1/3
Fe/H=3
Fe/H=3
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Importance of snow line
10-8Mo yr-1 6 x 10-8Mo yr-1 37/69
Major Challenges:
• Retention of grains: m-size barrier (Whipple)
• Fragmentation: km-size barrier (Benz)
• Planetesimal-growth barrier: Isolation mass barrier (Wetherill)
• Gas accretion barrier: critical-mass cores (Cameron)
• Retention of cores: type I migration (Goldreich &
Tremaine, Ward)
• Retention of gas giants: type II migration (Lin &
Papaloizou)
• Multiple gas giants: rapid depletion of disk gas
• Competing physics on multiple length & time scales
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Giant impacts and mergers
Liu Shangfei Zhou Jilin
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Enhanced formation of multiple planets
40/69 BeiBei Liu
XiaoJia Zhang
Grand design barrier: dynamical instability
• How did gas giants acquire their eccentricity?
Bryden
Jilin Zhou 41/69
Dynamical diversity
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Gas giants’ type II migration
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Beibei Liu
Core barrier: embryos’ resonant trapping
• Long term evolution: largest cores formed early
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Period distribution of hot Jupiters:
Dependence on stellar metallicity
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Smoking gun for core accretion (KOI 94)
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Planets’ size-period distribution from the Kepler surveys
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Type I migration with evolving disk
Transiting location move inward
Mass region corresponds to outward decrease slightly
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A
2 Earth Jupiter
½ Earth
5 Earth
r
critr
magr
starHot Jupiters park Closer than
Super Earths
Kretke
Gas giants SuperEarths
Neptunes
Sub/warm Earths
Super Earths: some key issues
• How to differentiate type I and II migration?
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Rai Xu, Wendy Ju
51/69 Zhuoxiao Wang Beibei Liu
New Candidate Catalog (Batalha et al. 2012) What can we learn from Multiple systems !!!
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How compact can multiple systems be?
Kevin Schlaufman Xiaojia Zheng
Stability and coplanarity
Random pairings
7.6% would be unstable x 742 pairs
= 56 unstable pairs
53/69 Fabricky
Super Earths: some key issues
• Did planets capture each other and parted their ways?
Exit resonances
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diverse migration mechanisms
Resonant capture Collisional damping Gas drag
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RM effect and challenge to migration
56/69 Liu, Guillichon
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Gas giants: some key issues
• Is there evidence for M * -dependent tidal dissipation?
Winn
Misaligned magnetosphere
Lai, Foucart, & Lin
Similar effects in close-in planets: additional Torque and dissipation avenues
Cumming & Lin Observable tests
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Alternative model: internal gravity wave
Tami Rogers 559/69
Gravity waves in intermediate-mass stars
60/69 Tami Rogers
Tami Rogers
Gas giants: some key issues
• Is there evidence for internal differential rotation ?
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62/69 Laine, De Colle
Inside the stellar magnetosphere
Inside the super Earths
Saur et al 63/69 B. Dai, Y.Z. Niu, R. Laine
Super Earths’ geology & atmosphere
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Other issues
Late-stage evolution in debris disks Post formation dynamical evolution Non planar planetary systems
Planets around different mass stars
The role of elemental differentiation in natal disks Planets in binary stars
Planets around stars in clusters
Planets’ magnetic and tidal interaction with their host stars Planets’ consumption by their host stars
Planets’ survival around evolved stars Planets’ internal structural evolution Planets’ atmospheric dynamics
How is habitability affected by dynamical interaction between planets
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Updated version of population synthesis models
66/69 Ida
67/69 Cosmographia 1544
Summary
• Planet formation is a robust process and their dynamical architecture is diverse.
• Planetary origin and destiny are determined largely by the structure & evolution of the disks.
• Migration due to planet-disk interaction played a big role in the asymptotic properties of the planets.
• Theory of planetary astrophysics is relevant to many other astrophysical contexts.
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