Planet Formation: theory and observations. Sean Raymond University of Colorado (until Friday) Observatoire de Bordeaux

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Transcription:

Planet Formation: theory and observations Sean Raymond University of Colorado (until Friday) Observatoire de Bordeaux

Outline Stages of Planet Formation Solar System Formation Cores to disks (c2d) Observational Constraints Formation and Evolution of Planetary Systems (FEPS)

Stages of Planet Formation

The Solar Nebula More volatile Available solids determined by disk temperature distribution and condensation temperatures

Stages of Planet Formation Type 1 migration Grains Planetesimals while gas remains Planetary Embryos No more gas Gaseous Planets Type 2 migration Dynamical instabilities Terrestrial Planets

Planetary Embryos (10 5-7 yrs) Gravitational focusing Runaway growth: dm/dt ~ M 4/3 (Safronov 1969) Large bodies excite small bodies: runaway ends when velocity dispersion of small bodies ~ v esc Depends on planetesimal size (Rafikov 2003; Chambers 2006) Oligarchic growth: dm/dt~πr 2 ~M 2/3 (Ida & Makino 1993, Kokubo & Ida 1998) Eccentricity Late-stage accretion starts when mass in large and small bodies is comparable (Kenyon & Bromley 2006) Semimajor Axis (AU) Kokubo & Ida 2002

Giant planet formation ( core accretion ) If embryos reach 5-10 M Earth before gas dissipates, can accrete nebular gas Core formation preferred just past snow line Credit: Phil Armitage

Planet migration in gaseous disks Type 1: low-mass planets Torques from density waves and co-rotating material Type 2: massive planets Carve gaps in disk, linked to disk s viscous evolution T viscous ~ 1 Myr Credit: Phil Armitage

Dynamical instabilities Exoplanet eccentricity distribution consistent with all systems going unstable Uncertainties: timing of instability (gaseous or gas-free environment?) Credit: Eric Ford

Late-stage terrestrial accretion Giant planets already formed (t gas ~ few Myr) Impacts from planetesimals and embryos Moon forming impact was last big one on Earth: 50-150 Myr (Touboul et al 2007) 1-10 Myr for last giant impact on Mars (Nimmo & Kleine 2007) (10 7-8 yrs)

Long-term dynamical evolution (Gyr) Small bodies cleared out by planets Planetary collision rates decreases rapidly (~power law) Late instabilities possible (e.g., Nice model ) Tsiganis et al 2005; Gomes et al 2005

Gas giants Earth -sized Runaway gas accretion Late-stage accretion planets Cores Embryos Planet e -simals (~km) Dust (µm) dust sticking Runaway growth Grav. collapse (cm - m) Oligarchic growth Late veneer 10 4-5 yrs 10 5-7 yrs 10 7-8 yrs

Solar System Formation

Gas giant planets Models can sort of reproduce Jupiter and Saturn (Chambers 2006, Thommes et al 2008) Uncertainties How to form 10 M E core in ~1 Myr? (Kenyon & Bromley 2009) Opacity (t form ~ κ 1/4 ) Gravitational instability? Chambers 2006

Raymond, Quinn & Lunine 2006

Terrestrial planet formation model Raymond, O Brien, Morbidelli, Kaib 2009 Caution: Jup, Sat not consistent with Kuiper Belt in these simulations

Observational Constraints: current and future

Can we constrain planetesimal and embryo formation? Need measurements of disk structure: Density Temperature Grain growth Turbulence? Johansen et al 2007

Protoplanetary Disk Lifetimes Disks last few Myr (Haisch et al 2001, others) Shorter-lived around binary stars (Cieza et al 2009) Last longer for lowermass stars (e.g., Pascucci et al 2009) BUT fewer gas giants around low-mass stars (Johnson et al 2007) M disk /M star ~ 1% (Andrews & Williams 2007) Mamajek 2009

Disk dissipation Disks cleared from the inside out or homologously (Currie et al 2009) Longer transition than previously thought (Simon & Prato 1995) Important for planet migration (Armitage 2007) Window for giant planet formation is 1-5 Myr (Currie et al 2009) 5 Myr old cluster NGC 2362 from Currie et al 2009

Uncertainties in giant planet Key measurements: Disk gas (rather than dust) Inner disk mass Radial Structure (snow line) formation Pascucci et al 2006

Planet migration Type 1: Turbulence T structure Resonant planets? Type 2: Dust from huge collision rates at inner resonances? Raymond, Mandell & Sigurdsson 2006

Dust (~planet formation timescales) in different radial zones 24 micron (1-10 AU) Meyer et al 2008 N Band (0.3-3 AU) Mamajek et al 2005 L Band (<0.1 AU) Haisch et al 2001

Models of dust production from accretion Dust in inner system decreases by ~10 Myr Colder dust evolves for 100s of Myr Reflects accretion and dynamical timescales Kenyon & Bromley 2005

24 micron dust brightness vs time Ramps up after few Myr Peaks at 10-30 Myr Slow decline at late times Broadly consistent with dust production from terrestrial planet formation (Kenyon & Bromley 2004) Currie et al 2008

Giant impacts Rare Increase dust by ~2 orders of magnitude Observed in HD 172555 (Lisse et al 2008) Mass (M Earth ) Log Time (yrs) Lisse et al 2008; Raymond et al (2006); Kenyon & Bromley (2005)

Dust belts HD 113766: 10-16 Myr F star with 3 dust belts 1.8 AU 4-9 AU 30-80 AU 20 year time span: requires dust replenishment from collisions Planetary influence on planetesimals? Lisse et al 2008

Raymond, Armitage, Mandell, Armstrong 2010

Link between free-floating planets and cold dust disks? Spitzer found three ~4 M J planets in 3 Myr old Sigma Orionis (Bihain et al 2009) Raymond, Armitage, & Gorelick 2009

Conclusions We have a good idea of the stages of planet formation Models and observations are mainly in agreement Observations that would really help planet formation models: Radial temp., density structure Turbulence

Thank you!