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Observations of HD189733b in Eclipse

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Nicmos allows objective mode spectro-photometry of transiting planets ... Substructure in the PSF. On scales of D/?, D/2? etc. Due to diffraction. D/? ~ 1/pixel ... – PowerPoint PPT presentation

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Title: Observations of HD189733b in Eclipse


1
Observations of HD189733b in Eclipse
  • G. Vasisht (JPL-Caltech) Collaborators

2
Spectroscopy from space
  • Nicmos allows objective mode spectro-photometry
    of transiting planets from 0.8-2.5 microns
  • On orbit effects make the photometry unstable for
    DR gt 103
  • Can it be made better?
  • Can the instabilities really be corrected
    ex-post-facto?

3
Introduction to NICMOS
  • Multipurpose NIR Instrument
  • Three cameras with NICMOS-3 focal planes
  • NIC3 has grisms G096, G141, G206
  • This talk G206
  • Exoplanet datasets have now been acquired with
    all grisms
  • G141 on HD 209548b (Brown et al. 2005)

4
Scientific Rationale
  • G206 range 1.45-2.55 microns
  • For transmission spectroscopy
  • Molecular transitions
  • Most species i.e. the hydrides of O,C,N,S or
    oxides have overtone or fundamental bands
  • Some immunity from scattering opacity
  • Reasonable contrast for T103 photospheres for
    dayside emission

5
Photometry with NICMOS
  • Differential is easier than absolute
  • Even so sources of error are a-plenty

Figer et al. 2004
6
Structure in the Response
NIC-3 is under-sampled Defocus provides
some Immunity For G206 this sets R 40
7
Structure in sub-Pixel Response
Finger et al. 2000
Stiavelli et al.
8
Photometry
Evaluate in some statistical fashion
9
Photometric errors
Variance depends on the power-spectral density of
the focal plane array Apodized by a filter
function
10
Diffraction
Intrapixel gain var
PSF
Defocused PSF by Ray Tracing Note this is a PSD
1-cos(k dx), dx 0.1 pix
11
What this means
  • Substructure in the PSF
  • On scales of D/?, D/2? etc
  • Due to diffraction
  • D/? 1/pixel
  • Scales with wavelength
  • For shorter ?, smaller scales
  • Can interact with subpixel structure

12
?
  • Beam wander
  • In x and y
  • Repositioning errors
  • Filter wheel positioning
  • Rot. about undeviated ray
  • PSF variation
  • Proxy Gaussian width
  • Array response variations
  • temperature of the detector
  • 1/K (2.5 micron), 3/K (1.5 micron)

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14
  • Nicmos data are of mixed quality
  • Troublesome first orbit
  • G206 versus G141
  • Positioning of the filter wheel
  • G206 positioning settles better?
  • with dx ? 0.1 pix versus 0.5 pix
  • smaller rotational errors in the dispersion
    axis

15
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16
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17
Pont et al.
18
F. Pont et al.
19
Orbit 1
20
Other Systematics
  • Optical effects
  • Flux-migration between grating-orders
  • Response of interference filter
  • Geometrical shadowing by grooves
  • Woods anomalies

21
State-Variables HD189733b
angle
position
defocus
temperature
22
Lightcurves
23
Noise
Light curve
Design Matrix
Model vector
24
Data Modeling-III
25
Spectral Modelling
  • Retrieval using RT models using well established
    scheme (Goody Yung 1989)
  • Disk-averaged radiative transfer models developed
    originally for Earthshine, Mars
  • (Tinetti et al. 2006, 2007)
  • Photochemistry (Caltech-JPL Kinetics model)
  • Layer-by-layer (log P between -6 and 0)
  • Input T-P profiles
  • Chemical profiles

26
HD189733b NIR Contrast Spectrum
27
Contrast Spectrum Components
28
Science Summary
  • Dayside emission
  • Water (ubiquitous, high VMR)
  • Carbon monoxide (thermochemically very stable at
    these P,Ts also Charbonneau et al. 2008)
  • Carbon dioxide (low VMR)
  • COH2O ?? CO2H2
  • COOH ?? CO2H
  • Methane upper limit
  • Residuals at the blue end of the spectrum
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