A HST/WFC3 Thermal Emission Spectrum of the Hot Jupiter HAT-P-7b

TL;DR

This study presents HST/WFC3 thermal emission spectra of the ultra-hot Jupiter HAT-P-7b, revealing a blackbody-like spectrum indicative of a thermal inversion and providing insights into its atmospheric composition and heat redistribution.

Contribution

First combined HST, Spitzer, and Kepler observations of HAT-P-7b, modeling its atmosphere with 3D GCM and 1D models to reveal thermal inversion and atmospheric properties.

Findings

HAT-P-7b's spectrum is well-fit by a blackbody at 2692 K.

The atmosphere exhibits a thermal inversion and weak heat redistribution.

Constraints on metallicity and C/O ratio suggest a near-solar composition.

Abstract

Secondary eclipse observations of several of the hottest hot Jupiters show featureless, blackbody-like spectra or molecular emission features, which are consistent with thermal inversions being present in those atmospheres. Theory predicts a transition between warmer atmospheres with thermal inversions and cooler atmospheres without inversions, but the exact transition point is unknown. In order to further investigate this issue, we observed two secondary eclipses of the hot Jupiter HAT-P-7b with the Hubble Space Telescope (HST) WFC3 instrument and combined these data with previous Spitzer and Kepler secondary eclipse observations. The HST and Spitzer data can be well fit by a blackbody with $T=2692 \pm 14$ K, and the Kepler data point constrains the geometric albedo to $A_{g}=0.077 \pm 0.006$. We modeled these data with a 3D GCM and 1D self-consistent forward models. The 1D models indicate that the atmosphere has a thermal inversion, weak heat redistribution, and water dissociation that limits the range of pressures probed. This result suggests that WFC3 observations of HAT-P-7b and possibly some other ultra-hot Jupiters appear blackbody-like because they probe a region near the tropopause where the atmospheric temperature changes slowly with pressure. Additionally, the 1D models constrain the atmospheric metallicity ($[\text{M/H}]=-0.87^{+0.38}_{-0.34}$) and the carbon-to-oxygen ratio (C/O $<1$ at 99 % confidence). The solar composition 3D GCM matches the Spitzer data but generally underpredicts the flux in the WFC3 bandpass and cannot reproduce its featureless shape. This discrepancy could be explained by high atmospheric drag or nightside clouds, and may be better understood through further observation with the James Webb Space Telescope (JWST).