Title: Extrasolar planets
1Extrasolar planets
2In this lecture
- Planets, Stars and Brown dwarves
- Recap planetary formation stages
- A missing population?
- Planet detection methods
- Radial velocity
- Transits
- Microlensing
- Direct Imaging
- Pulsar timing
- Astrometry
- Detection limits
- weird systems detected
- Giant branch stars
- Hot Jupiters
- Typical systems?
- Prevalence of planets
- Brown dwarf desert
- Orbital behavior
- The Future
www.exoplanet.eu
3Planets and Brown Dwarves
- Star
- Interstellar cloud collapse
- Burns hydrogen
- Mass gt 75 MJ
- Brown dwarf
- Interstellar cloud collapse
- Burns deuterium runs out fast
- Mass gt 13 MJ
- Jeans mass
- Determines the mass of the smallest
- object a collapsing cloud can form
- At T10K
- Densities not high enough to form
4Planetary Formation Stages Revisited
- Collapse of molecular cloud
- In lt 106 year
- Development of accretion disk
- Create central gap at stars co-rotation distance
- Form planetesimals
- Bodies grow by pair-wise accretion
- Self-gravity becomes important (r1km)
- Oligarchic growth of largest objects
- Gas Giant planets
- Cores of 10 ME capture large gas envelopes
- Opens gap in disk slowly migrates inward
- Gaseous component dissipates lt 10 Myr
5- Disk
- Gaseous component dissipates lt 10 Myr
- Debris disks remain 200 Myr
- Planets can migrate further by scattering small
bodies - Large collisions still frequent
6- Inner planets are composed of rock and iron
- Heated by radioactive decay
7- Gas giant planets Jupiter and Saturn
- Similar rock/ice cores of about 10 earth masses
- Large hydrogen envelopes molecular and metallic
- Ice Giant Planets Uranus and Neptune
- Rocky cores
- Water and Ammonia interiors
- Large hydrogen molecular envelopes
8- Another type of planet?
- We have a gap in our solar system
- An entire class of planet is unrepresented
?
- More than 10 Earth Masses results in a gas giant
- We know what planets in the 0-1 Earth Mass range
look like - What about the 1-10 Earth Mass range -
Super-Earths?
9Planetary Detection Radial Velocity
- Star and planet orbit systems center of mass
- Stars motion small compared to planets as M gtgt
MP - Star appears to approach and recede from us
periodically - Causes Doppler blue- and red-shifting of spectral
lines - Very precise spectral measurements needed
iodine cell - Current technology 1-3 ms-1
- Invert wavelength shift for velocity
- e.g. max velocity of the sun due to Jupiter is
12.5 ms-1 - In reality fit signal for period, MP sin(i) and
eccentricity - Cannot solve for inclination so mass is a lower
limit
- Star mass
- Stars bigger (hotter) than the sun not enough
absorption features - Stars smaller than the sun dont have a strong
signal - Technique sensitive to big planets with small
periods
10Planetary Detection Transits
- Planet passes in front of the star as seen from
Earth - Inclination must be close to 90º
- cos(i) lt (RRP)/a
- If a1AU, R1 solar radius then probability
0.4 - If a0.05AU, R1 solar radius then probability
8 - Limits on transit technique
- Brightness measurements precise to 0.1
- (RP/R)2 gt 10-3 or Rp gt 0.032 R
- e.g. for our solar system RPgt 22,000 km
- Gas/ice giants, not terrestrial planets
- Benefits of the transit technique
- Gives you a size
- All discoveries are good radial velocity
candidates - Gets you a mass (and mean density)
- Inclination is constrained
11Planetary Detection Direct Imaging
- 1AU separation at 1 parsec distance is 1
arc-second - Definition of a par-sec (3.086x1016 m)
- Angular separation is easy in ground-based
telescopes - Problem is the glare from the main star
- Use coronagraph
- Speckle imagery
- Longer wavelengths are better for contrast
- But worse for resolution
12- Other methods
- Microlensing
- Pulsar timing
- Supernova remnant
- Very precise but rarely used
- Astrometry
13Whats Detectable?
- Closer objects are easier
- Radial velocity
- Transits
- Pulsar timing
- Further objects are easier
- Astrometry
- Direct imaging
- Microlensing not affected by distance
-
- Heavy planets are always easier
- Greater tug on star
- Bigger signal easier to detect
- Current sensitivity limits up to gt MSATURN
- At reasonable distances from the star
- Current observational record of 10-15 years is a
big limitation - gt97 of these planets are within Jupiters
distance
14- Relative performance of various methods
www.exoplanet.eu
15- Were on the verge of an explosion in exoplanet
discovery rate
16Prevalence of Planets
- Population
- Total of 450 extrasolar planets
- Discovery rate 2 week-1
- Radial velocity searches show planets around 10
of stars - Stars are generally solar type
- Selection effect best signal / spectral feature
trade off - Planets are generally close in
- Selection effect most easily detected, short
observational record
- Most planets orbit metal rich(er) stars
- Metals for astronomers means Z gt 2
- The sun is also metal rich
17Geoff Marcys internet page.
Detection of weird systems
- Planets around supergiants
- Outward migration due to stellar mass loss
- Some planets do survive
- Many hot Jupiters
- Massive planets found close to star
- Pile up at periods of 4 days (0.05 AU)
- Can only be the result of orbital migration
- Large cores and gas envelopes require cool Ts
www.exoplanet.eu
18- What about these super-Earths
- Only two to talk about so far but there will soon
be many more
Uranus
Earth
www.exoplanet.eu
19Properties of Super-Earths
- Size vs Mass
- Size from transits
- Mass from radial velocities
- Equation of state needed to get size/mass
relation - Usually a non-unique solution
- This is a very simplistic approach
- With some knowledge of planetary science we can
eliminate a few possibilities
Swift et al., AstroPH, 2010
20- Super-Earths have a minimum radii
- Collision stripping can build super-Mercurys
- But material cant escape easily from such a
large planet - Theres no process that actually get you to a
pure iron planet - i.e. super-Earths are not like asteroids
Green 1/10 projectile/target Red1/4
projectile/target Blue 1/1 projectile/target
Earth
Pure iron
Marcus et al., ApJ 2010
21Properties of Super-Earths
- Plate tectonics?
- Earth yes
- Venus No
- What about bigger planets?
- Competing factors
- Higher gravity compresses and strengthens the
lithosphere - More vigorous convection more shear stress to
move and deform plates - Also, Faster convection means plates are younger
at subduction zones - Cooled enough (dense enough) to subduct?
22- Valencia et al. 2010
- Argues lithosphere will be thinner on larger
planets - Counters the strengthening due to gravity
- Super-Earths have plate tectonics
- Earth is borderline for plate tectonics in this
model - Requires wet conditions
Increasing shear stress
Dry
Wet
Fault strength vs planetary mass
23- Alternate viewpoint
- ONeill and Lenardic 2007
24- Two case examples
- CaRoT 7b
- GJ 1214b
- Both masses and sizes known
- A few other super-Earth planets where we only
have the mass are known
25- GJ1214b
- Mass 6.6 Earth Masses
- Radius 2.7 Earth Radii
- Density 1900 kg/m3
- Composition mostly water
- H/He envelope probably required
- Temperatures 450K
- Probably a very deep ocean
26- CaRoT7b
- Mass 4.8 Earth Masses
- Radius 1.7 Earth Radii
- Density Earth
- Composition is rocky
- Temperatures 2000K
- Plate tectonics here?
27The Story
4.5 Billion years
- Weve seen 400 years worth of this story 1st
hand - One ten millionth of solar system history
- Equivalent to watching 1 milli-second of a three
hour movie - Which we use to figure out the plot, the actors,
and what plays out at each location
28Dramaticus Personae
Volcanoes
Tectonics
Impact cratering
Eolian
Fluvial
Glacial
29On location
Mercury
Enceladus
Titan
Mars
30The Story
4.5 Billion years
- Weve seen 400 years worth of this story 1st
hand - One ten millionth of solar system history
- Equivalent to watching 1 milli-second of a three
hour movie - Which we use to figure out the plot, the actors,
and what plays out at each location
31Masses and the Brown Dwarf Desert
- Binary stars are common 50
- Initially controversial as to whether these
orbiting bodies were - Low mass binary companions (brown dwarves)
- Planets formed from an accretion disk
- Mass distribution is heavily skewed to lower
masses - Not (for once) a selection effect
- Low mass bodies are harder to detect yet we still
find more of them - Follows a power law
- Indicates large population of smaller objects
- The brown dwarf desert
- Few bodies between 10 and 80 MJ
- This low-mass population probably had a separate
formation mechanism
32Orbital Behavior
- 26 multiple planet systems
- E.g. Upsilon Andromedea
- Some with mean motion-resonances
- Hot-Jupiters/Neptunes
- Pile up at 4 day periods
- Eccentricities very small
- Tidal damping has been very effective
- Other systems
- Unusually high eccentricities
- Unexplained passing stars, disk interactions
- Eccentric gas giants are a problem for
terrestrial planets
33Physical Properties
- Not much to go on
- Future missions will provide spectra
- Planets that both transit and have radial
velocity measurements indicate gas giant
densities - Hot Neptunes now also known
- Overall understanding hasnt improved much in the
past 10 years - Modeling of expected atmospheric behavior yields
some exotic results
Gillon et al., 2007
34Future Missions
- Terrestrial Planet Finder (TPF)
- Direct imaging and spectra
- 1. Coronagraph
- 2. Interferometer
- KEPLER
- Transit observatory 1m mirror
- Launch 2009
- Monitor 105 stars for 4 years
- Space Interferometry Mission (SIM)
- Astrometric observatory
- 4 µ arcsec
- Will discover a lot of Jupiters
- Probably not terrestrial planets
- DARWIN
- ESA mission
- Direct imaging and spectra
35- Hopes for TPF and DARWIN
- Non-equilibrium component in atmospheres may be
signs of life
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37Planetary Detection Microlensing
- Planet and star pass in front of a background
star - Masses act as gravitational lenses
- Background star amplified
- Spread into Einstein ring (unresolved)
- Limitations
- Once off observation
- Lensing from planets lasts less than a day
- Retrieves mass, but not period
- Need dense background of stars
- E.g. galactic bulge
- Low mass planet detected
- 5.5 Earth mass around a cool red dwarf (a
super-Pluto)
Beaulieu et al., 2006
38Planetary Detection Pulsar Timing
- Neutron star with magnetic and rotational axes
unaligned - Rotation causes energetic beams to sweep through
space - We measure very regular radio pulses
- Pulsars are thought to be the best time-keepers
in the universe, but - some have pulses speeding up and slowing down
- Pulses take longer to travel here when the star
is further away - Rotation around a center of mass causes distance
changes - Pulse frequency oscillates with orbit
- Analogous to Doppler effect
- Technique also applied to pulsating white dwarves
- Very precise technique
- Can detect planets down to below 0.1 Earth Masses
- Smallest planet to date PSR 125712 b (2 Earth
Mass) - Drawbacks
- Pulsars are relatively rare
- Planets probably affected by supernovae blast
wave
39Planetary Detection Astrometry
- Look directly for positional shifting
- Remove effects of proper motion
- Angular motion given by
- E.g. Jupiter around the sun at 10pc 0.5
milli-arcsec - Doable with interferometers
- Most sensitive to large orbits
- but you have to wait a long time
- Good mass estimates but poor eccentricity
control - Still no planet detected this way
- but it can pin down inclinations of known planets
Benedict et al., 2002
40- Type I migration spiral density waves (fast)
- Torque exerted at Lindblad resonances
- Torque on outer disk is stronger than inner disk
- So planet migrates inwards on timescale
- Not very long!
- Type II migration gap opens (slower)
- Planet moves inward with the viscous gas
timescales of 106 years - Independent of planet mass
- Disk is truncated at the inner edge.
- Planets can stall there
Phil Armitages internet page.
- Close proximity high mass
- Ideal candidates for radial velocity and transit
obs - Transit gives sin(i) and size
- Radial velocity gives mass, eccentricity and
period - \We can get density values
- Objects are definitely gas giants
- Hot Neptunes now also discovered