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Characterizing Extrasolar Terrestrial Planets
Using Remote Sensing NASA
Astrobiology Institute
General Meeting 2003
March 11, 2003
David Crisp and Vikki Meadows
(VPL/JPL/Caltech)
2
Remote Sensing of Extrasolar Planet Environments
Radio
Infrared
VisibleUltra-Violet X-Ray
Gamma Ray
Once an extrasolar terrestrial planet has been detected and resolved from its parent star – All information about its
environment will arrive as photons
– This information can be decoded using remote sensing methods
3
Environmental Properties NeededExamples of factors affecting planetary habitability
• Global Energy Balance
– Stellar Type - luminosity, spectrum
– Orbital distance, eccentricity, obliquity, rotation rate
• In general, a planet with a moderately rapid rotation rate and low obliquity in a near circular orbit will have a more stable climate
– Bolometric albedo – fraction of stellar flux absorbed
• Presence of an atmosphere
– Surface pressure
– Bulk atmospheric composition
– Trace gases/greenhouse gases
– Clouds/aerosols
• Surface properties
– Presence of liquid water on the surface
• Surface pressure > 10 mbar
• Surface temperature > 273 K
– Land surface cover
How do we retrieve this information from planetary spectra?
?
4
Planetary Remote Sensing
O3
CH4
?
• A broad range of remote sensing techniques have been developed for studying Earth and other planets in our solar system – Photometry– Spectroscopy
• Extrasolar planets will pose special challenges– The planet will appear as an
unresolved point source• No direct constraints on size• No spatial details• Limited signal-to-noise
– No prospects for ground truth
5
Spectral Photometry
Photometric observations of a planetary disk in a few colors
• Can provide useful constraints on planetary properties, but …
• Sometimes yield ambiguous results– Not all pale blue dots are water worlds
with habitable environments– Not all red planets airless deserts– What does yellow-white mean?
Broad-band observations – provide constraints on the planetary
energy balance, but– Need independent constraints on the
SIZE of the body to quantify albedo, emissivity, and effective temperature
Twins?
6
Spectral Photometry
Photometric observations of an unresolved planetary disk are most useful when you know what you are looking for– Surface properties
• Chlorophyll red edge
– Atmospheric constituents• 0.76 m O2 A-band• 0.63 m H2O band• 9.6 m O3 band• 15m CO2 band
– Atmospheric and surface temperature• 15m CO2 band or other well-
mixed absorbing gas
CAUTION: Terrestrial planets are NOT black bodies!!
H2O
O2
O3
CO2
H2O
7
Time-Resolved Photometry
What can we learn from Time-resolved full-disk photometry (light curves)– Rotation periods– Variations in surface physical
properties• reflectance • thermal inertia
– Weather, climate and other time-variable phenomena• Large scale cloud systems• Regional/global dust storms
– Occultations could yield constraints on size• Large satellites• Background stars
(Lellouch et al. 2000)
Pluto Lightcurve
East Longitude
Flu
x (J
y)R
elat
ive
Alb
edo
100 200 3000
1.0
1.2
1.4
Central Meridian Longitude
Neptune Lightcurve
Solar
Thermal
8
Light Curves for the Earth
Issues:Clouds on an Earth-like terrestrial planet• Will reduce the
amplitude of the rotational lightcurve
• Can mask the rotation period
Goode et al. 2001: Earthshine Project
9
Spectral Remote Sensing
• Reflected Stellar Radiation– “Color” of the reflecting
surface (cloud top/ground)– Atmospheric pressure at the
reflecting surface – Column abundance of trace
gases– Clouds/aerosols
• Thermal Emission– Surface and atmospheric
thermal structure– Vertical distribution of
atmosphere temperatures and trace gases above the emitting surface• H2O, O3, CH4, N2O
H2OH2O
H2OH2O
O2
O3
H2ON2OCH4
CO2
O3
10
Characterizing Environments of Extrasolar Terrestrial Planets
• Once an extrasolar terrestrial planet has been detected (as an unresolved point source)– The first step will be to search for candidate
biosignatures in its spectrum
– If any are found, a more quantitative description of the planetary environment will be needed to determine whether they can be produced abiotically, or require a biological origin
8 10 12 14 16Wavelength (m)
O3?
GOT LIFE?
CO2?
11
Planetary Remote Sensing Using Reflected Stellar Radiation
• Optical properties of the reflecting surface (cloud deck/ground)– Albedo/emissivity
• Pressure of reflecting surface – Need a well-mixed gas with a known
spectrum is needed (e.g. O2 or CO2)
• Detection and quantification of column abundance of key trace gases - UV/VIS/near-IR– H2O, O2, O3, N2O, CH4, NH3 …
• Limitations– Little information about surface or
atmospheric temperatures
– Clouds preclude full-column or surface measurements
– Independent constraints on planet size essential, since albedos vary greatly
Cloud
12
Planetary Remote Sensing Using Thermal IR Emission
Thermal IR spectra can yield information about– Temperature of emitting surface
• Window regions– Atmospheric thermal structure
• Well-mixed gas: CO2 15 m band– Vertical distribution of temperatures and
trace gases above emitting surface• H2O, O3, CH4, N2O
Limitations– Atmospheric temperature information is
essential for retrieving trace gas amounts • requires a well-mixed gas with a known
spectrum
• Limited information on constituents near the surface – surface/atmosphere temperature gradient needed
– Thermal IR provides limited constraints on planetary surface composition
H2ON2OCH4
CO2
O3H2O
ThermalRadiation
Cloud
T(z)
13
Spectral Remote Sensing Algorithms
• Typical spectral remote sensing retrieval methods perform a constrained non-linear least squares fit of a function (synthetic radiance spectrum) to an observed spectrum.
• The fitting coefficients are the unknown atmospheric and surface properties that we are trying to retrieve – Surface albedo– Surface temperature and pressure– Atmospheric temperature profiles– Trace gas abundances and distributions– Cloud/aerosol composition, phase, optical depths
• Typical retrievals include the following steps– Initialize model with assumed surface and atmospheric
state - Assume a planet …– Calculate a synthetic spectrum, and compare it to the
observed spectrum– Perform a non-linear least square fit, solving for
atmospheric/surface state vector• Repeat process until the computed spectrum matches the
observations to within the convergence criteria
Alti
tud
e
H2 O
XH2O
aer
Alti
tud
e
T
Alti
tud
e
T(K)
14
Extracting Information from Spectral Remote Sensing Observations
• State Vector: Atmospheric and surface properties that affect the observed spectrum
• Forward Model: Computes the reflected or emitted spectrum for assumed state vector
• Instrument Model: Convolve results with Instrument Response function (spectral resolution, SNR, etc.)
• Inverse Model: Modify atmospheric and surface properties to improve fit
– “Radiance Jacobians” (weighting functions)• Give sensitivity of the spectral radiance at
each wavelength, i(), to variations in temperatures or optical properties in layer z
i(), i(), …. i()
Xj(z) Xj+1(z) T(z)– A priori Covariance Matricies: Provide Bayesian
constraints on the solution
FitTPF Obs
Alti
tud
e
H2 O aer T
Alti
tude
Xj Xj+1
H2 O
T(K)
aer T(K)
K = i/xj
Alti
tude
K = i/T
Typical remote sensing retrieval algorithms include:
15
Retrieval Algorithm Schematic
Atmospheric/ Surface State
Vector[Co2](z), PS,
T(z), Q(z), Ai(z),
Cj(z), a0()
Simulate Spectral Radiance
Forward Model:Radiance Spectra
Adjust The Atmospheric /Surface State
Inverse Model: Update State Vector
Final Atmospheric/surface StateXH2O, PS, T(z), A
i(z), Cj(z), A0()
ObservedSpectra
Convergence
Iter
atio
n Instrument Model
Tabulated OpticalProperties Of Gases,
Aerosols, Clouds
Aerosols, A1, A2, A3
H2O , 1, 2,, 3,…
CO2 , 1, 2,, 3…
16
Resolving Atmospheric Vertical Structure: Weighting Functions
Pre
ssu
re (
hP
a)
100
1000 0
10
5
15
Alt
itu
de
(km
)
GOES18 Channels
AIRS/CRIS>1000 Channels
Wavelength (m)5.010.015.0 3.4
300
260
220
Brig
htn
ess
Tem
per
atur
e (K
)
Different spectral regions are sensitive to different levels of the surface -atmosphere system. The vertical resolution for temperature and trace gas retrievals increases with spectral resolution and signal-to-noise.
17
Effects of Spectral Resolution on Retrieval Accuracy
The accuracy of Temperature and trace constituent retrievals increases as the spectral resolution and measurement signal-to-noise ratio increases.
18
Special Challenges Posed by Extrasolar Terrestrial Planets
While reliable remote sensing retrieval methods exist for studying terrestrial planets in our solar system, extrasolar terrestrial planets pose unique challenges
– Spatial variations: • Most existing remote sensing retrieval methods
can be applied only to soundings acquired over a spatially homogeneous scene
• The first generation observations of terrestrial planets will provide only disk integrated results that mix viewing geometries, surface types, clear and cloudy scenes, etc.
– Additional (ad-hoc) constraints will be needed to define the spatial variability within each sounding
– Modest spectral resolution and signal / noise• resolving power < 100
• Signal-to-noise ratios <<100
19
Unresolved Spatial Variability
Spatial variability over the disk of an unresolved planet introduces challenges– Signal comes primarily from the
brightest areas - not a true disk average
• Reflected Stellar Radiation:– Highest surface albedos at visual
and near infrared wavelengths (clouds, polar caps)
• Thermal wavelengths:– Warmest regions
– Observations of variability over diurnal and seasonal cycles will help to constrain spatial variations
20
Unresolved Spatial Variability
Contributions from different parts of the disk traverse different atmospheric paths
• Thermal: Longer paths near limb• Solar: path increases with solar
incidence or emission zenith angles
• Absorption by gases and airborne particles is proportional to the product of the optical pathlength and the absorber amount:
= N(z) (,z) dz
– if the optical pathlength is unknown, we can’t retrieve unique estimates of the trace gas abundances.
– Ad-hoc constraints may be needed (especially if temperatures and absorber amounts vary)
21
Impact on Retrieval Algorithms
• Unresolved spatial variability introduces two specific challenges for existing remote sensing retrieval algorithms
– Forward model: Even though only disk-averaged observations are available, synthetic radiances must be generated for an array of points on the planet’s disk to:• Resolve spatial variability in surface or
atmospheric properties• Accommodate variations is atmospheric
pathlengths over different parts of disk
– Inverse Method: Radiance Jacobians also vary spatially across the disk, and must be computed on a spatially resolved grid because
½ i(,,) / Xj(z,,) sin d d ≠
½ / Xj(z) i( ,,) sin d d
22
Boot-Strap Method
• Assume a spatially-varying description of planetary properties– Couple the retrieval model to a climate model and other ad hoc
assumptions• Calculate spatially-resolved radiances and radiance Jacobians
– Integrate radiances over the disk and compare to observations– Integrate radiance Jacobians over disk to predict 0th order
correction to assumed atmospheric and surface properties• Derive new estimates of state structure variables
– Constrained by climate model or ad-hoc assumptions• Repeat until the retrieval converges
This approach is underconstrained and will result in a family of equally-likely solutions…..
23
Implications for TPF and DarwinVIS Coronagraphs• Most trace gas information is at UV and
near-IR wavelengths– Currently ignored in TPF designs
• Time dependent photometric or spectroscopic data may be essential to detect/discriminate biosignatures
IR Nulling interferometers• Atmospheric temperatures must be
measured to quantify trace gas amounts from thermal radiances– A well mixed gas with a well known
spectrum is essential for this– The CO2 15 micron band is the best
candidate for terrestrial planets in our solar system (Venus/Earth/Mars)
• Moderate spectral resolution and high signal-to-noise are essential for characterizing environments
• The problem is still underconstrained