An HST/WFC3 thermal emission spectrum of the hot Jupiter HAT-P-7b
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 inversi...
Huvudupphovsmän: | , , , , , , , , , |
---|---|
Materialtyp: | Journal article |
Publicerad: |
American Astronomical Society
2018
|
_version_ | 1826296041614344192 |
---|---|
author | Mansfield, M Bean, JL Line, MR Parmentier, V Kreidberg, L Désert, J-M Fortney, JJ Stevenson, KB Arcangeli, J Dragomir, D |
author_facet | Mansfield, M Bean, JL Line, MR Parmentier, V Kreidberg, L Désert, J-M Fortney, JJ Stevenson, KB Arcangeli, J Dragomir, D |
author_sort | Mansfield, M |
collection | OXFORD |
description | 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 ± 14 K, and the Kepler data point constrains the geometric albedo to A g = 0.077 ± 0.006. We modeled these data with a three-dimensional (3D) GCM and one-dimensional (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 ($[{\rm{M}}/{\rm{H}}]=-{0.87}_{-0.34}^{+0.38}$) 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. |
first_indexed | 2024-03-07T04:10:15Z |
format | Journal article |
id | oxford-uuid:c794f6a3-8e60-4386-be96-6b3846c2f00a |
institution | University of Oxford |
last_indexed | 2024-03-07T04:10:15Z |
publishDate | 2018 |
publisher | American Astronomical Society |
record_format | dspace |
spelling | oxford-uuid:c794f6a3-8e60-4386-be96-6b3846c2f00a2022-03-27T06:46:12ZAn HST/WFC3 thermal emission spectrum of the hot Jupiter HAT-P-7bJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:c794f6a3-8e60-4386-be96-6b3846c2f00aSymplectic Elements at OxfordAmerican Astronomical Society2018Mansfield, MBean, JLLine, MRParmentier, VKreidberg, LDésert, J-MFortney, JJStevenson, KBArcangeli, JDragomir, DSecondary 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 ± 14 K, and the Kepler data point constrains the geometric albedo to A g = 0.077 ± 0.006. We modeled these data with a three-dimensional (3D) GCM and one-dimensional (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 ($[{\rm{M}}/{\rm{H}}]=-{0.87}_{-0.34}^{+0.38}$) 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. |
spellingShingle | Mansfield, M Bean, JL Line, MR Parmentier, V Kreidberg, L Désert, J-M Fortney, JJ Stevenson, KB Arcangeli, J Dragomir, D An HST/WFC3 thermal emission spectrum of the hot Jupiter HAT-P-7b |
title | An HST/WFC3 thermal emission spectrum of the hot Jupiter HAT-P-7b |
title_full | An HST/WFC3 thermal emission spectrum of the hot Jupiter HAT-P-7b |
title_fullStr | An HST/WFC3 thermal emission spectrum of the hot Jupiter HAT-P-7b |
title_full_unstemmed | An HST/WFC3 thermal emission spectrum of the hot Jupiter HAT-P-7b |
title_short | An HST/WFC3 thermal emission spectrum of the hot Jupiter HAT-P-7b |
title_sort | hst wfc3 thermal emission spectrum of the hot jupiter hat p 7b |
work_keys_str_mv | AT mansfieldm anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT beanjl anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT linemr anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT parmentierv anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT kreidbergl anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT desertjm anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT fortneyjj anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT stevensonkb anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT arcangelij anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT dragomird anhstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT mansfieldm hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT beanjl hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT linemr hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT parmentierv hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT kreidbergl hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT desertjm hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT fortneyjj hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT stevensonkb hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT arcangelij hstwfc3thermalemissionspectrumofthehotjupiterhatp7b AT dragomird hstwfc3thermalemissionspectrumofthehotjupiterhatp7b |