Characterization of Exoplanets in the mid-ir with JWST & ELTs

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Characterization of Exoplanets in the mid-ir with JWST & ELTs Jupiter HR8799 Saturn VLT/ISAAC VLT/NACO Cassini/VIMS Wolfgang Brandner (MPIA), Eric Pantin (CEA Saclay), Ralf Siebenmorgen (ESO), Carolina Bergfors (MPIA), Sebastian Daemgen (ESO), Kerstin Geißler (SUNY Stony Brook), Markus Janson (Univ. of Toronto)

Why study Exoplanets in the Mid-IR?

The challenge in direct studies of exoplanets extreme flux ratio between star and planet small angular separation (!1 ) Direct detections require high precision measurements: high contrast, high signal-to-noise, high angular resolution,... => differential imaging, secondary transits, mid-ir observations

Mid-IR fluxes of directly imaged exoplanets Name Dist [pc] Sep Mass Teff[K] H [mag] Flux(L ) HR8799b 39.4 1.72 7 MJup 870 17.8 0.14mJy HR8799c 39.4 0.96 10 MJup 1090 16.9 0.33mJy HR8799d 39.4 0.62 10 MJup 1090 16.8 0.39mJy FomalhautB 7.7 12.7 2.5 MJup: 400: >22.9 <0.06mJy Beta Pic b 19.3 0.4 8 MJup 1500? 7.48mJy Marois et al. 2008 Current sample of directly imaged exoplanets represents the tip of the iceberg : large angular separations, massive & young

Mid-IR instruments & Synergies (10000s, 10!) => see poster by Bernhard Brandl + beta Pic B + HR 8799d + HR 8799c + HR 8799b GMT E-ELT TMT Synergies: JWST: better point source sensitivity ELTs: up to 6.5 times higher angular resolution at same wavelength JWST: better suited for time-critical observations (transits,...) ELTs: higher spectral resolution JWST-NIRCAM => JWST will be more sensitive towards lower mass (cooler) exoplanets in wider orbits => ELTs will be more sensitive for direct imaging detections of exoplanets in closer orbits

E-ELT/METIS discovery space E-ELT/METIS could directly image a 1 MJup planet in a 1 AU orbit around a 5 Gyr old G2V star at 5 pc (wavelength: 8.6"m, integration time: 3600s, 4-quadrant phase mask)

Observations of ultra-cool atmospheres Probing the unexpected

A cloudy picture - standard model of cool atmospheres Cloud condensations remove species from the higher atmospheric layers (no metal-oxides in L-dwarfs, no Li in T-dwarfs, etc.) ~125 K 600-1200 K 1200-2000 K ~2200 K d c Model assumptions trace of planet c spectra? Katharina Lodders, 2004 (Science) stratification (absence of pronounced vertical mixing) deeper layers are hotter (no temperature inversion) chemical equilibrium local thermal equilibrium

Spectral analysis of exoplanet atmospheres The ultra-cool brown dwarf ULAS J0034-00 (Teff ~ 550K) b d flux (arb. units) H2O CH4 1.0 5.0 10.0 wavelength (!m) Leggett et al. 2009 => models reproduce spectral features of cool brown dwarfs reasonably well => see also poster by Micaela Stumpf

Probing exoplanet atmospheres Observations of the secondary eclipse of the transiting exoplanet TrES-4 with SPITZER/IRAC (Knutson et al. 2009):

Probing exoplanet atmospheres H2O emission best fit standard planetary atmosphere thermal inversion 3.6 to 8.0 µm observations of TrES-4 reveal temperature inversion in exoplanet atmosphere (Knutson et al. 2009)!

HD 189733: 200 AU K-M binary HD 189733A hosts the transiting exoplanet HD 189733b HD 189733b is tidally-locked (P=2.2d) hot Jupiter, Teff = 1100 K, M=1.15 MJup, with H2O, CH4 and CO2 in its atmosphere secondary-transit spectroscopy

fluorescent methane Swain et al. 2010 Saturn s northern aurora LTE atmospheric models cannot explain spectral features => models with non-local thermal equilibrium required

HR 8799: A5V, 1.5MSun, d=38 pc, age " 60 Myr b c ~8 MJup d 8 MJup 10 MJup ~10 MJup 10 MJup trace of planet c spectra? ~10 MJup Marois et al. 2008

HR 8799: A5V, 1.5MSun, d=38 pc, age " 60 Myr b c d 8 MJup 10 MJup Marois et al. 2008 10 MJup trace of planet c spectra? HR 8799b: ~8 MJup, T = 800 K HR 8799c & d: ~10 MJup, T = 1100 K

L -band spectroscopy of the directly imaged exoplanet HR 8799c Observing run in October 2009 with VLT/NACO: 4 x 0.5 nights b Strategy: use long-slit, place both the star and one of the planets in the slit nod along the slit every 100s, integrate for 10000s per half night d c L =15.6mag (0.14 mjy, S/N! 30) L =14.7mag HR 8799c,10 MJup, Teff = 1100K tint = 10 000s L =5.2mag trace of planet c spectra? 1 planets detected in 300s imaging (!0.4s with E-ELT/METIS) 3.8 wavelength ["m] 4.2

MIR measurements constrain atmospheric properties: VLT/NACO observations of HR 8799c more CO, less CH4 than expected => non-equilibrium chemistry

Summary: Science Goals mid-ir: optimal contrast planet/star + study of intrinsic thermal emission of exoplanets (direct imaging detections & secondary transits) Scientific topics addressed by direct detections of giant exoplanets in the mid-ir: Exoplanet orbital parameters (astrometry) * * Atmospheric composition and chemistry * Temperature profile * Internal structure (radius, mass) * Weather and seasons * Formation of giant planets (core accretion, disk instability)

Dynamical simulation of the HR 8799 system 1.5 MSun 10 MJup 10 MJup 7 MJup stable orbits

Dynamical simulation of the HR 8799 system 40 MJup 28 MJup 40 MJup unstable system with chaotic orbits