AI summary · arXiv: 2611.14703v1 · astro-ph.EP

Dwarfs of Fire and Ice: UV-Irradiation-Driven Thermal Inversion, Disequilibrium Chemistry, and a Cloud-Free Atmosphere in a Strongly Irradiated Brown Dwarf Probed by JWST/NIRSpec Phase-Resolved Spectroscopy

Lael Shin, Daniel Apai, Yifan Zhou, Joshua D. Lothringer, Daphne Broski-Laing, Sarah L. Casewell, Siyi Xu, Ben W. P. Lew,
and 5 more authorsXianyu Tan, Jenni R. French, Vivien Parmentier, Mark S. Marley, L. C. Mayorga
Original paper Submitted to arXiv on 10 Nov. 2026 Accepted for publication in ApJ on November 5, 2026. 25 pages, 16 figures License: CC BY 4.0

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The essentials

JWST phase-resolved spectra of SDSS1411B reveal a dayside thermal inversion, likely CO2 disequilibrium, weak heat redistribution, and spectra adequately modeled without clouds.

Question

How does intense UV irradiation from a white dwarf shape the atmospheric structure, chemistry, and energy transport of its brown-dwarf companion? The study uses broad-wavelength phase-resolved spectroscopy to investigate these effects in SDSS1411B.

Method

The authors analyzed 2.27 hours of JWST/NIRSpec PRISM observations covering 0.6–5.3 μm across the binary’s approximately 2.02-hour orbit, using 75 integrations. They modeled phase curves with a second-order Fourier series, compared spectra with equilibrium forward models, and performed joint retrievals across the night, morning, and day using 80 pressure layers and MultiNest with 1,000 live points.

Findings

  • Authors’ interpretation The Fourier-model amplitudes correlate with molecular-opacity regions, which the authors interpret as evidence for larger flux variations in upper atmospheric layers.
  • Result The preferred retrieval finds a prominent dayside temperature inversion, with the inversion occurring at a different pressure on the morning side.
  • Result Retrievals favor free CO2 chemistry over equilibrium chemistry, especially because the free-CO2 model better reproduces the nightside feature near 4 μm.
  • Result Adding clouds did not significantly improve the retrieval, and the cloudless model was statistically preferred.
    See the passage in the paper
    We also found that including cloud components does not significantly improve the spectral fit relative to the cloudless model (Figure 7), despite the increased model complexity.
  • Result The energy-budget analysis indicates heat-redistribution efficiency below 0.1 for the assumed zero-albedo case, while the inferred cooling age and radius differ in their consistency with evolutionary models.

Limitations

  • The energy-budget calculation relies on simplifying assumptions, including how irradiation is absorbed and how energy is distributed between hemispheres.
    See the passage in the paper
    We note that our simple model does not specifically consider the potential complication that some UV flux is absorbed and thermally re-emitted in the upper atmosphere; this would have an effect similar to a higher Bond Albedo even though it would not be from scattering.
  • The spectra do not directly exclude nightside clouds, so the cloudless result means clouds are not required by these data rather than proving their absence.
    See the passage in the paper
    One caveat in the above scenario is that the observed spectrum does not directly rule out the presence of clouds on the nightside.
  • The conclusions concern one system; the authors state that a broader sample is needed to establish how irradiation affects cloud formation across brown dwarfs.
    See the passage in the paper
    Systematic cloud analyses based on broad-wavelength spectroscopy of a larger sample of irradiated BDs will therefore be essential for determining how external irradiation influences phase-dependent cloud formation.

Why it matters

The authors argue that SDSS1411B occupies an important irradiation regime: it is the least strongly irradiated brown dwarf known in their comparison to show a substantial dayside inversion. Its phase-resolved spectra demonstrate how JWST observations of white-dwarf–brown-dwarf binaries can probe irradiation-linked thermal structure and disequilibrium chemistry.

Written by AI from the paper. Passages are checked word for word against the text we analysed; the rest may contain errors.

AI-generated keywords: White dwarf–brown dwarf binary Ultraviolet irradiation Atmospheric temperature inversion Disequilibrium chemistry Heat redistribution

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  • Comprehensive Summary
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  • Original abstract
The paper investigates how intense ultraviolet irradiation from a white dwarf affects the atmosphere of its close brown-dwarf companion, SDSS1411B. It examines whether irradiation alters the brown dwarf’s temperature structure, chemistry, clouds, and day-to-night energy transport. With an orbital period of about two hours and an incident flux of approximately 10^8.6 erg s−1 cm−2, the system provides an intermediate-irradiation case among close white-dwarf–brown-dwarf binaries. It also offers a way to study effects that are difficult to isolate in ordinary brown dwarfs or star–planet systems. The study uses 2.27 hours of JWST/NIRSpec PRISM time-series observations, covering 0.6–5.3 micrometers over a complete orbit. The authors reduced and flux-calibrated the spectra, modeled the primary and secondary eclipses to refine the orbital timing, and separated the nearly steady white-dwarf spectrum from the brown dwarf’s variable emission. They fitted the brown dwarf’s phase curves with second-order Fourier models and compared the reconstructed dayside, morning-side, and nightside spectra with non-irradiated atmosphere models and multi-phase atmospheric retrievals. The retrievals allowed flexible temperature–pressure profiles and compared equilibrium chemistry with models that permitted variable carbon dioxide abundances, as well as models with and without clouds. The observed variability depends strongly on wavelength. Outside eclipses, the system varies by less than 2 percent at 0.6–1.47 micrometers, where white-dwarf light dominates, but by about 54 percent in the 4.40–5.20 micrometer band. The brown dwarf’s integrated dayside flux is about 280 percent greater than its nightside flux. Brightness temperatures range from roughly 600 to 2,000 K, with a mean day–night temperature difference of about 610 K. The largest differences, around 1,000 K, occur near 3 and 5 micrometers. The fitted light curves have nearly zero phase offset, suggesting that the hottest region lies close to the substellar point. The authors interpret this result as evidence of limited longitudinal heat transport rather than strong zonal advection. Non-irradiated equilibrium forward models do not reproduce the observed spectra, particularly the dayside emission features near 3 and 5 micrometers. The preferred retrieval fits the spectra better, finding a monotonic nightside temperature profile but temperature inversions on the morning side and dayside. The dayside inversion occurs near 0.1 bar, while the morning-side inversion occurs near 1 bar. The authors suggest that ultraviolet-rich radiation from the white dwarf heats the upper atmosphere, potentially aided by reduced water-vapor cooling if water dissociates. Irradiated one-dimensional models with a hot white-dwarf spectrum produce a qualitatively similar inversion, whereas a comparison model irradiated by a cooler, Sun-like star does not. This result supports, but does not prove, the proposed ultraviolet-heating explanation. The retrieval statistically favors a cloud-free model and a freely fitted carbon dioxide abundance over equilibrium chemistry. Clouds are not required by the data. Although the cloudy model implies low optical depth, the observations do not rule out clouds, particularly on the nightside. The retrieved nightside carbon dioxide abundance exceeds the equilibrium prediction, while the dayside abundance is lower, possibly because of thermal or photochemical dissociation. These chemical explanations remain hypotheses; the processes themselves are not directly detected. An energy-budget analysis yields effective temperatures of about 1,703 K on the dayside and 1,272 K on the nightside. Under the authors’ assumptions, the heat-redistribution efficiency is below 0.1.

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