Characterizing exoplanets’ atmospheres and surfaces Thérèse Encrenaz LESIA, Observatoire de Paris Pathways Toward Habitable Planets Barcelona, 14-18 September 2009
Mar 27, 2015
Characterizing exoplanets’ atmospheres and surfaces
Thérèse EncrenazLESIA, Observatoire de Paris
Pathways Toward Habitable Planets
Barcelona, 14-18 September 2009
Outline
• The planetary zoo• Rocky Exoplanets (warm)
– Spectral variations with spectral type, RH, abundances – Atmosphere: constraints on resolving power– Surface: mineralogy, Red Vegetation Edge
• Icy Exoplanets (cold)– Atmosphere: constraint on R– Surface: ices
• Giant Exoplanets (from hot to very cold)– Atmosphere: importance of thermal profile, constraint on R
• Conclusions
Spectroscopy of an exoplanet
• Reflected starlight component (UV, visible, near-IR)– Albedo is about 0.3 for most of solar-system planets– Absorption lines or bands in front of stellar blackbody
• Thermal component (IR, submm & mm)– Mostly depends upon the temperature of the emitting region– Emission lines in the stratosphere, absorption lines in the troposphere
(function of T(P)) • Fluorescence emission (UV, visible, near-IR)
– Emission lines in the upper atmospheres (H, H2, N2, radicals)
• The IR range is best suited for probing exoplanets’ neutral atmospheres
The Solar System: A planetary zoo• Planets with an atmosphere• Rocky planets (warm)
– Mars-type (CO2, N2 + H2O) No stratosphere– Earth-type (N2, O2 + H2O) Stratosphere (O3)
• Icy planets (cold)– Titan-type (N2, CH4 + CO) Stratosphere (hydrocarbons, nitriles)
• Giant planets (cold to very cold)– Jupiter-type (H2, CH4, NH3 +H2O) Stratosphere (hydrocarbons)– Neptune-type (H2, CH4) «
• Bare planets – Mercury/asteroid-type (refractories) – TNO-type (ices)
Te (K) 1200 850 460 220 120 50Stellar distance (AU) 0.05 0.1 0.3 1.5 5.0 20.0(solar-type star)Small Exoplanet < ROCKY PLANETS > <ICY PLANETS >
(WARM) (COLD)
(0.01 - 10 ME) No atmosphere Atmosphere Atmosphere
(Mercury-type) N2, CO2, CO, H2 N2, CH4(+CO)
(Mars-Venus type) hydrocarbons, nitrilesif O2 -> O3 (Earth-type) (Titan-type)STRATOSPHERE STRATOSPHERE
Giant Exoplanet <PEGASIDES>< GASEOUS GIANTS > <ICY GIANTS> (HOT) (WARM) (COLD)
(10 - 1000 ME) Atmosphere Atmosphere Atmosphere
H2,CO,N2,H2O H2,CH4,NH3,H2O H2,CH4
hydrocarbons hydrocarbons (Jupiter-type) (Neptune-type)STRATOSPHERE STRATOSPHERE
What kind of exoplanet can we expect? [F*/D2](1-a) = 4 Te4
Te (K) 1200 850 460 273 220 120 50
Stellar typeA 0.15 0.3 0.9 3.0 4.5 15.0 60.0(T=10000 K)F 0.08 0.16 0.5 1.6 2.4 8.0 32.0(T=7000 K)G 0.05 0.1 0.3 1.0 1.5 5.0 20.0(T=5700 K)K 0.04 0.12 0.4 0.6 2.0 8.0(T=4200 K)M 0.04 0.14 0.2 0.4 1.4(T=3200 K)
HZ
Variations of asterocentric distances with the stellar type
However, this is not so simple! Why?
• Other parameters are involved:– Albedo -> effect on Te– Rotation period -> effect on Te
• Phase-locked planets -> strong day/night contrasts
– Possible greenhouse effect -> may increase Ts vs Te• Earth: 15 K; Venus: over 200 K
– Obliquity• Atmospheric dynamics -> may change day/night contrasts
– Magnetic field -> may prevent atmospheric escape
• Migration is possible!
Rocky PlanetsThe IR spectrum of Mars (ISO-SWS)
Spectral signatures: CO2, H2O, CO (+ traces H2O2, CH4)
H2O
CO2 CO2
COCO2
Lellouch et al., 2000
Hydrated silicates
CO2
Ps = 6 mb
Variation of a Mars-type spectrum as a function of the stellar type (D = 1 UA)
StellarTypeA(10000 K)
F(7000 K)
G(5700 K)K(4200 K)
Te (K)
476
346
273
174
Variation of a Mars-type spectrum as a function of the asterocentric distance D
(solar-type star)
D = 0.07, 0.1, 0.3, 1.0 UATe = 1000, 863, 496, 273 K
NB: For small D, the reflected component dominates-> Atmospheric signatures mostly in absorption
Variation with atmospheric composition: H2O-dominated (Earth-like) spectrum (above clouds)
H2O H2O
H2O CO2
CO2
H2Oice
Pcl = 10 mb
The infrared spectrum of the Earth as seen by the NIMS instrument aboard Galileo (Earth flyby, December 1990)
Drossart et al., 1993
The thermal spectrum of telluric planets
Venus
Earth
Mars
Hanel et al., 1992
Thermal spectra of rocky planets
Resolving power required :CO2 = 3 m R = 3O3 = 1 m R = 10CH4 = 0.15m R = 50
EarthMarsVenus
EarthR=70,10,5
Hanel et al., 1992
Solid signatures in rocky planets
Mid-latitudesTsurf > Tatm
Polar capTsurf < Tatm
Silicates: 1000 - 1200 cm-1(broad)Water ice: 700 - 900 cm-1 (broad)
Reflected spectrum: H2O ice 1.25, 1.5, 2.0 mSilicates 1.0, 2.0 m (broad)Ferric oxides 1.0 m Carbonates 2.35, 2.5 mHydrated silicates 3.0-3.5 m (broad)
Thermal spectrum:
H2O ice
silicates
The Red Vegetation Edge (Earth spectrum)
Seager et al. 2005
RVE : Earthshine observations
Seager et al. 2005
Problems:-partial coverage of the vegetation-clouds (20-30% ofthe disk)
The reflected spectrumof a CH4-dominatedplanet(icy or giant)
Larson, 1980
The atmosphere of an icy planet:The thermal component
Titan - SWS: CH4, hydrocarbons, nitriles
Resolving power required: R > 5 ( C2H2-C2H6) ; R > 10 (CH4)
CH4
C2H6
HCN, C2H2
Solid signatures on icy planets
H2O ice H2O, CH4, CO, N2
(Ganymede) (Pluto)
The atmosphere of two gaseous giants: The thermal component Jupiter & Saturn - ISO-SWS
CH4
CH3D, PH3 NH3
C2H6
Jupiter
Saturn
NB: Jupiter and Saturn are VERY different!
PH3
Jupiter -SWS The 6-12-m range: CH4, CH3D, C2H6, NH3, PH3
Resolving power required:- for NH3 detection: R > 100- for CH4 detection: R > 150-for C2H6 detection: R > 20
The atmosphere of an icy giant Neptune - SWS The 2-18- range: CH4, CH3D, C2H2, C2H6
Resolving power required: R > 5 ( C2H2-C2H6) ; R > 10 (CH4)
CH4 C2H6 C2H2
In summary…
• The diversity in solar-system bodies opens the same possibilities for exoplanets
• A resolving power higher than 10 is required for the identification of major gaseous and solid signatures
• In the thermal range, hydrocarbons (C2H2, C2H6) are easier to detect than methane
• Knowing the thermal structure is essential for interpreting thermal spectra
• No stratosphere expected for Rocky Exoplanets (N2, CO2, H2O) except if O2 is present
• A stratosphere is expected for Icy Exoplanets (N2, CH4) and Giant Exoplanets (H2, CH4,…)