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Measuring the Astrometric Signature of Transiting Planets with SIM Scott Gaudi, Ohio State University

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  • Measuring theAstrometric Signatureof Transiting Planets

    with SIMScott Gaudi, Ohio State University

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  • Order of Magnitude

    • Centroid:

    • Uniform surface brightness, full transit:

    • Amplitude of the centroid shift:

    !"x =#*$x I( $x , $y )d $x d $y%%I( $x , $y )d $x d $y%%

    , !"y =#*$y I( $x , $y )d $x d $y%%I( $x , $y )d $x d $y%%

    !"x=#*

    $

    1%$x, !"

    y=#*

    $

    1%$y, where $ =

    Rp

    R*

    &

    '(

    )

    *+

    2

    is the transit depth

    !

    !T "#*$

    1%$& 2.5µas

    Rp

    RJ

    '

    ()

    *

    +,

    2

    R*

    R"

    '

    ()

    *

    +,

    %1

    d

    20pc

    '

    ()

    *

    +,

    %1

  • Astrometric Wobble and Transit Signal• HD 189733• M*=0.81M, R*=0.79R, d=19.3pc• Mp=1.15MJ, Rp=1.16RJ, a=0.031AU• Astrometric Wobble Amplitude

    • Astrometric Transit Amplitude

    • Ratio of Amplitudes

    • Ratio of Durations

    !

    !T "#*$

    1%$& 2.5µas

    Rp

    RJ

    '

    ()

    *

    +,

    2

    R*

    R"

    '

    ()

    *

    +,

    %1

    d

    20pc

    '

    ()

    *

    +,

    %1

    !

    !W "a

    d

    M p

    M* +Mp# 1.9µas

    a

    0.04AU

    $

    %&

    '

    ()Mp

    MJ

    $

    %&

    '

    ()M*

    M"

    $

    %&

    '

    ()

    *1

    d

    20pc

    $

    %&

    '

    ()

    *1

    !

    !T

    !W

    " 1 Rp

    RJ

    #

    $%

    &

    '(

    2

    R*

    R"

    #

    $%

    &

    '(

    )1

    a

    0.04AU

    #

    $%

    &

    '(

    )1M

    p

    MJ

    #

    $%

    &

    '(

    )1

    M*

    M"

    #

    $%

    &

    '(

    Period of Orbit

    Transit Duration=!a

    R*

    ~ 30

  • Parameter Dependence• Transit Duration

    • Parallel Amplitude

    • Perpendicular Amplitude

    Duration = 2!0(1" b

    2)

    1/2, where !

    0#PR

    *

    2$a

    ~!T(1" b

    2)1/2

    ~!Tb

  • Observable Parameters

    • Photometric

    • Astrometric

    b, r !Rp

    R*

    , t0, "

    0

    b, r !Rp

    R*

    , t0, "

    0, #

    *, $

    !

    φ = angle of projected planet orbit normal w.r.t. sky coordinates

  • What is it good for?

    • Measure M* and R*.• Measure Mp and Rp.• Confirm or constrain polarized reflected

    light measurements.• Determine the inclination of the planet orbit

    w.r.t. more distant companions.• Remove degeneracies is multiple transiting

    planets systems.

  • Signal-to-Noise Ratio and Uncertainties

    • Signal-to-Noise Ratio– Duration decreases with b– Signal amplitude increases with b

    • Parameter Uncertainties– Assume photometric parameters

    are known– Fisher matrix

    S

    N=Q

    2

    3(1! b2 )1/2 (1+ 2b2 )

    "

    #$%

    &'

    1/2

    , Q ( ()*0)1/2 +T

    ,

    !

    "#* /#* ~ "$ ~ (S /N)%1

  • Known Systems• Estimated S/N per transit

    pair– 10% Out-of-transit data– Two transits with

    orthogonal baselines– Four V=10 ref. Stars– Three chop cycles– 30s integrations

    • Also S/N for 30 total hrs– Three systems with S/N>3

    • GJ436b, S/N~7.3• HD189733b, S/N~16.9• HD209458b, S/N~3.9

    – Three with 1.5

  • To Do

    • Practical application.– Refined S/N estimates.– Suitable reference stars?– Optimal strategies.– Expected uncertainties.

    • Additional systems?• Astrometric signature of eclipsing binaries.