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Solving the Puzzles of Planet Formation in the Era of K2, TESS and PLATO

Solving the Puzzles of Planet Formation in the Era of K2, TESS and PLATO

A colloquium I gave at the University of Birmingham in the UK. The idea what to show what we can learn from terrestrial planet formation, conditioned on Kepler data.

Tom Barclay

July 10, 2016
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  1. Tom Barclay
    NASA Ames Research Center
    University of Birmingham
    July 11, 2016
    Solving the Puzzles of Planet Formation
    in the Era of K2, TESS and PLATO

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  4. 4
    How do Planets Form?

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  5. Collapse of molecular cloud core proto-star + disk
    (Shu, Adams, & Lizano 1987)
    Planets Form From Disks

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  6. Early stage
    dust grains planetesimals
    ~ μm ~1-10 km
    • non-gravitational sticking process
    remains poorly understood
    Classical Solar Nebular Theory

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  7. Early stage
    dust grains planetesimals
    ~ μm ~1-10 km
    Middle stage
    planetesimals planetary embryos
    ~103 km
    Kokubo & Ida 2002
    Classical Solar Nebular Theory

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  8. Early stage
    dust grains planetesimals
    ~ μm ~1-10 km
    Middle stage
    planetesimals planetary embryos
    ~103 km
    Late stage
    embryos planets
    Classical Solar Nebular Theory

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  9. Planetary systems are diverse!
    3300 planets in 560 systems as of today (2300 discovered with Kepler)

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  10. Exoplanet Detections, 2015
    Earth
    >4600 Candidates

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  12. N-body Models
    Challenges:
    1. Models assume perfect accretion (fragmentation increases N)
    2. N-body systems are chaotic, need lots of simulations
    My modeling work addresses these two issues
    Mercury modified to
    include state-of-the-art
    collisions model
    We performed hundreds
    of N-body simulations to
    infer results statistically
    Chambers (2013)
    Quintana, Barclay et al. 2016 (arxiv 1511.03663)
    Barclay et al, submitted to ApJ

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  13. rimp


    B
    B rimp
    rtar
    rtar
    θ
    θ
    ℓ = rtar
    + rimp
    - B
    ℓ = 2 rimp
    vimp
    vimp
    (a)
    (b)
    New Collision Model
    Based on model by
    Stewart & Leinhardt (2012)
    Mercury N-body integration package modified to include
    collision model that maps outcomes of a two-body
    collisions based on masses and impact geometry
    Outcomes include:
    -collision with central star, giant planet
    -perfect accretion
    -fragmentation
    -hit-and-run collisions (Asphaug 2006)
    Chambers (2013)
    Quintana, Barclay et al. 2016
    (arxiv 1511.03663)

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  14. Quantities We Can Track
    Time of final giant impact

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  15. Giant Siblings

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  16. Jupiter analogs are likely scarce!
    Occurrence Rates of Jupiter (RV + Transits) ~ 6%
    (Wittenmyer et al. 2016)

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  17. Effect of Giant Planets on Formation of
    Earth-like Planets
    Case 1: Sun + Jupiter + Saturn
    Case 2: Sun only (no giants)
    Disk model: 26 (lunar) embryos, 260 (Mars) planetesimals
    Smallest fragments = 0.5 lunar mass
    300 simulations, each for 2 Gyr where all bodies fully
    interact gravitationally and collisionally,

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  18. Jupiter+Saturn
    18
    No giant planets

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  19. 19
    Simulations

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  20. Results from Early Tests

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  21. We can use Modern Statistics
    Final giant impacts
    happen earlier if there
    are giant planets

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  22. 22
    WFIRST is going to be
    searching for
    free-floating planets.
    How many will it find?

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  23. 23
    Outer disk is
    ejected first
    Efficient radial mixing
    with no giant planets
    Fragments from
    inner system
    ejected later
    Dependence on Initial Semimajor Axis

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  24. 24
    WFIRST will find
    plenty of Mars’ but
    few earths
    If Giant planets
    are rare,
    WFIRST finds
    no FFP
    WFIRST Detections

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  25. 25
    Sun-Only

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  26. 26
    Micro-Oort Clouds?

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  27. Planets Orbiting
    Cool Stars

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  28. G dwarf
    M dwarf
    Kepler-186
    Sun
    Detecting Planets around
    M dwarfs is Easier
    TIME
    BRIGHTNESS
    BRIGHTNESS
    TIME

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  29. Kepler-186f
    Quintana, Barclay et al.

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  30. Finding if Earth-analogs can form in these regimes
    has big implications for the abundance of life in
    the Universe
    7 out of 10 stars in our galaxy are M dwarfs

    Most stars lack outer giant companions

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  31. Raymond et al. 2007
    Earth’s have been
    found around M stars
    of all sizes!!

    This assumption of
    disks cannot be true
    Planet Formation around Cool Stars
    TRAPPIST-1
    M = 0.08 Msun
    Kepler-186
    M = 0.5 Msun

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  32. Kepler-186 Example
    We can form Earths around
    Kepler-186 if we use high mass disk
    (15 M⨁
    within 0.5 AU) and steep
    surface density profile

    These types of disks aren’t predicted
    To resolve this: Invoke migration?

    We can use N-body simulations as a
    forward model to create synthetic
    catalogs: compare with Kepler/K2/
    TESS/PLATO observed catalogs
    My future research will explore how Earth’s form
    around low mass stars

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  33. Modeling Collisions Critical for M star
    Regime!
    My work will investigate these characteristics
    Shorter orbital periods
    High speed impacts
    Accreting and retaining
    water, atmospheres is
    more difficult

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  34. Giants Planets
    Orbiting
    Giants Stars

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  35. We can use asteroseismology to
    infer stellar properties
    We can use Gaussian Processes
    to get around increased noise
    from granulations
    K2 will observe 100,000+giants
    TESS will observe millions
    If red giant occurrence rates
    match main-sequence stars, TESS
    will find 1000s. BUT…
    We can learn the occurrence
    rates for planets around red
    giants
    Main Sequence star
    Red giant star
    Chaplin et al 2013

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  36. We can use asteroseismology to
    infer stellar properties
    We can use Gaussian Processes
    to get around increased noise
    from granulations (to search as
    well as model)
    K2 will observe 100,000+giants
    TESS will observe millions
    If red giant occurrence rates
    match main-sequence stars, TESS
    will find 1000s. BUT…
    We can learn the occurrence
    rates for planets around red
    giants Barclay et al 2015

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  37. We can use asteroseismology to
    infer stellar properties
    We can use Gaussian Processes
    to get around increased noise
    from granulations
    K2 will observe 100,000+giants
    TESS will observe millions
    Huber et al 2016

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  38. We can use asteroseismology to
    infer stellar properties
    We can use Gaussian Processes
    to get around increased noise
    from granulations
    K2 will observe 100,000+giants
    TESS will observe millions
    If red giant occurrence rates
    match main-sequence stars, TESS
    will find 1000s. BUT…
    We can learn the occurrence
    rates for planets around red
    giants
    Barclay et al, in prep

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  39. We can use asteroseismology to
    infer stellar properties
    We can use Gaussian Processes
    to get around increased noise
    from granulations
    K2 will observe 100,000+giants
    TESS will observe millions
    If red giant occurrence rates
    match main-sequence stars, TESS
    will find 1000s. BUT…
    We can learn the occurrence
    rates for planets around red
    giants

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  40. Takeaways
    A. We can use observations to place constraints on planet
    formation models.
    B. From models we can learn about planet formation and
    evolution: composition, water delivery, impact history.
    C. Planets are heavily influenced by their siblings. We must
    think in terms of planetary systems.
    D. M-dwarfs are the first places we will search for life. We
    can predict what we will find and inform strategies.
    E. Planets around red giants provide unique laboratories
    that teach us about our own future.
    F. We can combine observations, theory and modern
    statistics.

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