stsci may symposium 2005
DESCRIPTION
Phil Armitage (University of Colorado). Migration. Migration regimes Time scale for massive planet formation Observational signatures. Ken Rice (UC Riverside) Dimitri Veras (Colorado). + Mario Livio, Steve Lubow & Jim Pringle. STScI May Symposium 2005. Migration. - PowerPoint PPT PresentationTRANSCRIPT
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STScI May Symposium 2005
MigrationPhil Armitage (University of Colorado)
Ken Rice (UC Riverside)Dimitri Veras (Colorado)
Migration regimesTime scale for massive planet formationObservational signatures
+ Mario Livio, SteveLubow & Jim Pringle
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STScI May Symposium 2005
Gravitational perturbation from planet
Exchange of angular momentum with gas or particle disk
Change in orbit - migrationmigrationPerturbation to the disk surface density
http://ciclops.lpl.arizona.edu/
Migration
Described as Type I / Type II migrationdepending on whether perturbationis weak / strong
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STScI May Symposium 2005
http://ciclops.lpl.arizona.edu/
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STScI May Symposium 2005
QuickTime™ and aYUV420 codec decompressor
are needed to see this picture.
Migration regimesSlowly increaseMp - compute theresponse of a 2Dlaminar diskType I - small effect on disk, ~Earth masses
Type II - gap opening at ~Jupiter mass
Displayed in an almost corotating frame
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STScI May Symposium 2005
Type I migration and planet formationIs Type I migration important for:
Assembling giant planet cores M ~ 20 MEarth
Terrestrial planet formation M << MEarth
Rate can be calculated analytically:
€
T ∝M p2 ⇒ tmigrate ∝M p
−1Net torque
Tanaka, Takeuchi & Ward (2002)
€
vmigratevKepler
≈ −3qrp
2Σ
M*
h
rp
⎛
⎝ ⎜ ⎜
⎞
⎠ ⎟ ⎟
−2q = Mp / M*
h / r is diskthickness
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STScI May Symposium 2005
For a minimum mass Solar Nebula profile:
€
vmigrate ~ 1× M p M⊕( ) cm/s VERY FAST!
Analytic estimatein agreement with simulations byBate et al. (2003)
No reason tobelieve that
Type I migrationdoesn’t occur
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STScI May Symposium 2005
Criticalcore mass~20 MEarth
Migration time scale
of 50 Myr (10 x disk)
Time scale of 1 Myr
Migrationdominated
Migrationmatters forgiant planetcoresHourigan & Ward 84Alibert et al. 04
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STScI May Symposium 2005
Type I migration: laminar disks
Expect fast growth up to isolation mass
At isolation in same disk model, Type I rate matters at all radii
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STScI May Symposium 2005
Turbulent disk: scattering off fluctuations will dominate Type I rate at low enough masses
Diffusive migration regime - planet will random walk in a
Simulations: Nelson & Papaloizou (2004)Laughlin, Steinacker & Adams (2004)
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STScI May Symposium 2005
core
/ t
ota
l m
ass
Could reduce core mass + formation time scales (Rice & Armitage 2003)
Important for terrestrial planet formation??
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STScI May Symposium 2005
Type II migration
Coupled evolution of planet + disk
Inward at small r, outward at large r
Uncertainty: poorly known disk physics
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STScI May Symposium 2005
Type II migration
Coupled evolution of planet + disk
Inward at small r, outward at large r
Uncertainty: poorly known disk physics
QuickTime™ and aGIF decompressor
are needed to see this picture.How lossy is the planet formation process?
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STScI May Symposium 2005
r = 0.1au Bell et al. (1997)
10-8 Msun / yr
10-7 Msun / yr
Can exclude in situ formation only for the small fraction of hot Jupiters: Tdisk > 1600K
dust destruction
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STScI May Symposium 2005
Is Type II migration common?Expect Type II migration if:
Planets form significantly prior to gas dispersal
Disk evolves (accretion)
€
Mdisk t form( ) ≥ M p
Can we find evidence for migration in the statistical distribution of extrasolar planets: N(Mp,a,e,[Fe/H]…)?Models: Trilling et al. (1998); Armitage et al. (2002); Trilling, Lunine & Benz (2002); Ida & Lin (2004a,b)
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STScI May Symposium 2005
Distribution of planets with orbital radius is consistent with a maximal migration model:
Planets form at `large’ radii ~5 auMigrate inwardSwallowed by star, unless stranded during migration by disk dispersal
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STScI May Symposium 2005
Raw census of extrasolar planets in dN / dlog(a)
Selection effects + multiple surveys
Cumming et al. (1999); Udry et al. (2003); Jones et al. (2004)
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STScI May Symposium 2005
Distribution of planets with M > MJ
only
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STScI May Symposium 2005
Predicted distributionfrom migrationonly - Armitageet al. (2002)
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STScI May Symposium 2005
Not unique - may be able to identify better signatures using extra information from host star metallicity
Observationally and theoretically, planet formation via core accretion becomes much easier at higher [Fe/H] or p
If we assume that [Fe/H] differences are the main source of variations in p(r), present host metallicity tells us how quickly cores formed at different radii
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STScI May Symposium 2005
Schematically:
Hoststar’s[Fe/H]
log(a)
Core forms quickly:substantial migration
Core forms just as thegas is about to be lost:little or no migration
Lower envelope of planets in [Fe/H] - a plane defines a sample of objects predicted to suffer less than average migration
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STScI May Symposium 2005
Critical metallicity curve depends upon planet formation model (e.g. amount of Type I migration) + surface density profile of disk
No Type I migration: Rice & Armitage ‘05
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STScI May Symposium 2005
Simple core accretion models (cf Ida & Lin 04)including slow Type I migration of the core
Measurement of critical [Fe/H] as f(a) from large planet samples at a ~ few au could constrain core accretion models
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STScI May Symposium 2005
SummaryStochastic migration of very low mass bodies from scattering off turbulent fluctuations
Type I migration rate is fast - will impact growth of giant planet cores
Expect Type II migration to be common - future observations may confirm statistical clues that it really happened