Cloud busting: enstatite and quartz clouds in the atmosphere of 2M2224-0158

Author:

Burningham Ben1ORCID,Faherty Jacqueline K2,Gonzales Eileen C12345,Marley Mark S6,Visscher Channon78,Lupu Roxana69,Gaarn Josefine1,Fabienne Bieger Michelle110ORCID,Freedman Richard611ORCID,Saumon Didier12

Affiliation:

1. Centre for Astrophysics Research, Department of Physics, Astronomy and Mathematics, University of Hertfordshire, Hatfield AL10 9AB, UK

2. Department of Astrophysics, American Museum of Natural History, New York, NY 10024, USA

3. Department of Astronomy and Carl Sagan Institute, Cornell University, 122 Sciences Drive, Ithaca, NY 14853, USA

4. The Graduate Center, City University of New York, New York, NY 10016, USA

5. Department of Physics and Astronomy, Hunter College, City University of New York, New York, NY 10065, USA

6. NASA Ames Research Center, Mail Stop 245-3, Moffett Field, CA 94035, USA

7. Department of Chemistry, Dordt University, Sioux Center, IA 51250, USA

8. Space Science Institute, Boulder, CO 80301, USA

9. Bay Area Environmental Research Institute, 625 2nd Street, Suite 209, Petaluma, CA 94952, USA

10. College of Engineering, Mathematics and Physical Sciences, University of Exeter, North Park Road, Exeter, UK

11. SETI Institute, Mountain View, CA 94043, USA

12. Los Alamos National Laboratory, P.O. Box 1663, MS F663, Los Alamos, NM 87545, USA

Abstract

ABSTRACT We present the most detailed data-driven exploration of cloud opacity in a substellar object to-date. We have tested over 60 combinations of cloud composition and structure, particle-size distribution, scattering model, and gas phase composition assumptions against archival 1–15 μm spectroscopy for the unusually red L4.5 dwarf 2MASSW J2224438-015852 using the Brewster retrieval framework. We find that, within our framework, a model that includes enstatite and quartz cloud layers at shallow pressures, combined with a deep iron cloud deck fits the data best. This model assumes a Hansen distribution for particle sizes for each cloud, and Mie scattering. We retrieved particle effective radii of $\log _{10} a {\rm (\mu m)} = -1.41^{+0.18}_{-0.17}$ for enstatite, $-0.44^{+0.04}_{-0.20}$ for quartz, and $-0.77^{+0.05}_{-0.06}$ for iron. Our inferred cloud column densities suggest ${\rm (Mg/Si)} = 0.69^{+0.06}_{-0.08}$ if there are no other sinks for magnesium or silicon. Models that include forsterite alongside, or in place of, these cloud species are strongly rejected in favour of the above combination. We estimate a radius of 0.75 ± 0.02 RJup, which is considerably smaller than predicted by evolutionary models for a field age object with the luminosity of 2M2224-0158. Models which assume vertically constant gas fractions are consistently preferred over models that assume thermochemical equilibrium. From our retrieved gas fractions, we infer ${\rm [M/H]} = +0.38^{+0.07}_{-0.06}$ and ${\rm C/O} = 0.83^{+0.06}_{-0.07}$. Both these values are towards the upper end of the stellar distribution in the Solar neighbourhood, and are mutually consistent in this context. A composition towards the extremes of the local distribution is consistent with this target being an outlier in the ultracool dwarf population.

Funder

European Commission

NSF

NASA

Science and Technology Facilities Council

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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