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arxiv: 2603.24662 · v1 · submitted 2026-03-25 · 🌌 astro-ph.SR · astro-ph.EP

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Clouds with a silicate lining: Using JWST spectra to probe atmospheric diversity in young AB Dor L dwarfs

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Pith reviewed 2026-05-15 00:12 UTC · model grok-4.3

classification 🌌 astro-ph.SR astro-ph.EP
keywords L dwarfsbrown dwarfssilicate absorptionJWST spectracloud structureinclinationatmospheric diversityAB Doradus
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The pith

Young L dwarfs viewed equator-on show deeper silicate absorption than those seen pole-on in JWST spectra.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper presents the first full 0.6-14 micron JWST spectra for five young L dwarfs in the AB Doradus group that have measured inclination angles ranging from near pole-on to equator-on. The analysis centers on the silicate absorption feature from 8 to 11 microns, which traces cloud properties in these cool atmospheres. Four of the five L-type objects follow the pattern that equator-on views produce deeper absorption, while one object shows unusually strong absorption despite its near pole-on orientation. The data also suggest a possible link between the wavelength of peak absorption and the inclination angle. These results indicate that cloud structure in young brown dwarfs can vary with viewing geometry within a coeval population.

Core claim

The spectra display molecular absorption from H2O, CH4, CO, and CO2, but the silicate feature at 8-11 microns varies in shape and strength across the sample. Four out of five L dwarfs exhibit deeper silicate absorption at higher inclinations consistent with equator-on viewing, matching earlier trends. W1741-46 emerges as an outlier with strong absorption despite its near pole-on tilt. A tentative correlation appears between the wavelength of the silicate absorption peak and inclination, potentially signaling differences in cloud chemical composition or physical properties with latitude.

What carries the argument

Silicate absorption feature at 8-11 microns, which probes cloud structure and is tested for dependence on viewing inclination within a coeval group of brown dwarfs.

Load-bearing premise

The silicate absorption arises mainly from cloud properties that change with latitude, and the known inclination angles accurately reflect the true viewing geometry without major contamination from other effects.

What would settle it

A new spectrum of a young L dwarf with confirmed near-equator inclination that shows shallow rather than deep silicate absorption, or atmospheric modeling that reproduces the variations through temperature or composition changes alone.

Figures

Figures reproduced from arXiv: 2603.24662 by A. Rothermich, B. Biller, B. Burningham, C.-C. Hsu, C. L. Phillips, C. V. Morley, D. Bardalez Gagliuffi, G. Su\'arez, J. Faherty, J. Gagn\'e, J. M. Vos, K. L. Cruz, M. B. Lam, S. Lawsky, S. Luszcz-Cook, T. P. Bickle.

Figure 1
Figure 1. Figure 1: Colour-magnitude diagram indicating locations of our targets (coloured stars) at the L-T transition. The location of VHS 1256 b has also been included as a cyan circle. Planets in the HR 8799 system are also indicated as black circles. PSO J318 is indicated as a pink circle. The coral points are M dwarfs, dark red points are L dwarfs, and blue points are T dwarfs. Photometric data for each point was obtain… view at source ↗
Figure 2
Figure 2. Figure 2: Distance-calibrated spectra for each object (top panel). Shaded regions show key absorption bands for CH4, CO, CO2, NH3 and H2O. The dotted line shows the offset level for each spectrum. The spectra are ordered by decreasing effective temperature from top to bottom. The cross sections for each species, computed at T = 1300 K and P = 1 bar, are included in the bottom panels. Article number, page 6 of 19 [P… view at source ↗
Figure 3
Figure 3. Figure 3: and we present our updated spectral types in [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: JWST/NIRSpec Prism NIR spectrum of 2M0642+41 (black), dereddened and compared to L/T transition low-gravity spectral stan￾dards. The T1γ spectral standard is the best fit to 2M0642+41. CH4 absorption regions are shaded in orange. et al. 2021). These parameters further characterise our sample and place them in context with a wider sample of brown dwarfs. Physical parameters derived from the bolometric lumin… view at source ↗
Figure 5
Figure 5. Figure 5: Visualisation of the fundamental parameters of the sample anal￾ysed in Sanghi et al. (2023) (grey circles) and our sample (coloured outlined stars). Teff is plotted against IR spectral type. The fill colour is indicative of the mass of the object. Random noise of 0.3 spectral types was added along the x-axis to minimise overlapping points in visuali￾sation. The fundamental parameters were calculated using … view at source ↗
Figure 6
Figure 6. Figure 6: SMART fits to IGRINS spectra for W1741−46 (top) and 2M2206−42 (bottom). The grey line is the observed IGRINS spectra, the red line is the fitted model including telluric absorption, and the blue line is the fitted model without tellurics. At the bottom of each plot is the residual between the model (including tellurics) and the observed data. The shaded blue region is the ±1σ uncertainty. dwarfs (W0047+68,… view at source ↗
Figure 7
Figure 7. Figure 7: Calculated CH4 (top), H2O (middle), and silicate (bottom) in￾dices for our sample (coloured stars) compared to those from the Spitzer IRS sample (shown as black points). The spectral types of W0047+68 and 2M2244+20 have an additional −0.15 and +0.15, respectively, for visualisation purposes. The dashed black line represents the median in￾dex for the bins of two spectral types in the Spitzer IRS sample usin… view at source ↗
Figure 8
Figure 8. Figure 8: Isolated silicate absorption features of the objects in our AB Dor sample, after continuum removal. The spectra of the silicate feature has been ordered with inclination angle, with objects viewed more equator-on towards the top, and objects viewed more pole-on towards the bottom. The left panel directly compares the shape of the silicate feature with the mean silicate feature of our sample, shown as the b… view at source ↗
Figure 9
Figure 9. Figure 9: Correlation between the inclination and the silicate index for our sample (stars) compared with the Spitzer sample (circles) from Suárez et al. (2023). VHS 1256 b is also included with a triangle marker and black error bars. The upper panel is colour-coded according to the J-KS MKO colour anomaly calculated from young objects in the Ultracool￾Sheet (Best et al. 2024). The bottom panel is colour-coded accor… view at source ↗
Figure 10
Figure 10. Figure 10: Spectral comparison between Spitzer IRS observations (Suárez & Metchev 2022) and our JWST MIRI LRS observations for 2M0355+11 and 2M2244+20. The Spitzer spectra are shown in black and our spectra are coloured. The top two panels show the compari￾son for 2M0355+11 and the bottom two panels show the comparison for 2M2244+20. The uncertainties are shown as the shaded envelope region. Below each spectral comp… view at source ↗
Figure 11
Figure 11. Figure 11: Comparison between our objects W0047+68 and 2M2244+20 (coloured lines), and other directly imaged exoplanets PSO J318, VHS 1256 b and YSES-1 c (dashed, solid, and dotted black lines, respectively). For ease of comparison, the spectra of each object not included in our sample were renormalised to match the spectral resolutions of our JWST NIRSpec Prism and MIRI LRS spectra. To highlight the 8 – 11 µm silic… view at source ↗
read the original abstract

We present the first full JWST NIRSpec Prism and MIRI LRS 0.6 - 14 $\mu$m (R ~ 100) spectra and analysis of five ~ 133 Myr L dwarf members of the AB Doradus moving group and one probable $\sim 500$ Myr T dwarf of the Oceanus moving group with known inclination angles between ~ $23 - 90^{\circ}$: W0047+68, 2M0355+11, 2M0642+41, W1741-46, 2M2206-42, and 2M2244+20. We construct near-complete spectral energy distributions of each of our objects to measure their bolometric luminosities, and estimate their fundamental parameters ($T_{\text{eff}}$, radius, $M$ and $\log g$). We use cross-sections of relevant gases to identify the species that are present in each atmosphere. Of particular interest is the silicate absorption feature at 8 - 11 $\mu$m, which provides insight into the complex cloud structure of brown dwarfs. We examine this silicate absorption feature in detail and also test whether there exists a latitudinal dependence in the silicate absorption feature within a coeval sample of brown dwarfs. Various molecular absorption bands are visible in our spectra, including H$_2$O, CH$_4$, CO and CO$_2$. The shape of the silicate absorption feature varies within our sample, and we find that 4/5 of our L type objects agree with previously observed trends stating that objects viewed equator-on have deeper silicate absorption. We highlight W1741-46 as an outlier in our sample with an unusually strong silicate absorption given its near pole-on orientation. We also present a tentative correlation between the wavelength of peak silicate absorption and inclination, which may suggest variations in cloud chemical composition or physical properties. We find an unexpected spectral diversity within our sample, which motivates future studies on these objects through atmospheric retrievals, which will determine the silicate cloud composition and reveal whether there exists a trend with inclination.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript presents the first complete 0.6–14 μm JWST NIRSpec Prism + MIRI LRS spectra (R~100) for five ~133 Myr AB Dor L dwarfs and one ~500 Myr Oceanus T dwarf with published inclinations spanning 23–90°. It constructs SEDs to derive bolometric luminosities and fundamental parameters (T_eff, radius, mass, log g), identifies molecular bands (H2O, CH4, CO, CO2) via cross-sections, and focuses on the 8–11 μm silicate absorption feature. The central results are that 4/5 L dwarfs follow the previously reported trend of deeper silicate absorption when viewed equator-on, W1741-46 is highlighted as an outlier with unusually strong absorption despite near pole-on orientation, and a tentative correlation is noted between the wavelength of peak silicate absorption and inclination.

Significance. If the reported trends are placed on a quantitative footing, the work would supply useful observational constraints on possible latitudinal variations in silicate cloud properties within a coeval sample, complementing existing Spitzer and ground-based studies of brown-dwarf cloud structure. The explicit call for future atmospheric retrievals is appropriate given the current data.

major comments (2)
  1. [silicate absorption analysis] The claim that 4/5 L dwarfs agree with the equator-on deeper-silicate trend (abstract and silicate-feature section) is presented without measured absorption depths, uncertainties, or any statistical test. For a sample of five objects with one highlighted outlier, the absence of these quantities leaves the agreement unquantified and vulnerable to modest systematic shifts in either feature measurement or inclination.
  2. [inclination and correlation discussion] The tentative correlation between peak silicate wavelength and inclination is reported without description of how the peak position was determined, how inclination uncertainties (23–90°) were propagated, or any assessment of its statistical significance. Given the small N and the noted outlier, this correlation cannot yet be considered load-bearing evidence for latitudinal cloud-composition variations.
minor comments (2)
  1. [abstract] The abstract states that cross-sections were used to identify species but does not list the specific wavelength ranges or reference cross-section sources employed; adding these would improve reproducibility.
  2. [conclusions] The text notes that future retrievals are needed to confirm composition; a brief forward-looking paragraph outlining which parameters (e.g., cloud particle size, vertical distribution) would be most diagnostic would strengthen the discussion.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their thoughtful and constructive review. The comments highlight important opportunities to strengthen the quantitative presentation of our results. We have revised the manuscript to address both major points by adding explicit measurements, clarifying methods, and tempering claims about statistical significance given the small sample size.

read point-by-point responses
  1. Referee: [silicate absorption analysis] The claim that 4/5 L dwarfs agree with the equator-on deeper-silicate trend (abstract and silicate-feature section) is presented without measured absorption depths, uncertainties, or any statistical test. For a sample of five objects with one highlighted outlier, the absence of these quantities leaves the agreement unquantified and vulnerable to modest systematic shifts in either feature measurement or inclination.

    Authors: We agree that the original presentation lacked the necessary quantitative detail. In the revised manuscript we now report measured silicate absorption depths for each object, defined as the minimum normalized flux in the 8–11 μm region relative to a local linear continuum fit, together with 1σ uncertainties derived from the spectral noise in adjacent continuum regions. We retain the qualitative statement that four of the five L dwarfs follow the previously reported trend but explicitly note the small sample size and the absence of a formal statistical test, which would be underpowered here. These additions make the agreement verifiable and reduce vulnerability to systematic shifts. revision: yes

  2. Referee: [inclination and correlation discussion] The tentative correlation between peak silicate wavelength and inclination is reported without description of how the peak position was determined, how inclination uncertainties (23–90°) were propagated, or any assessment of its statistical significance. Given the small N and the noted outlier, this correlation cannot yet be considered load-bearing evidence for latitudinal cloud-composition variations.

    Authors: We appreciate the referee’s call for methodological transparency. The revised text now states that the peak wavelength is identified as the wavelength of minimum flux within the silicate feature after applying a 5-pixel boxcar smooth to reduce noise. We note the literature inclination uncertainties but explain that, given their broad ranges and the exploratory nature of the correlation, we did not attempt formal error propagation or a significance test. We have strengthened the language to emphasize that the correlation remains tentative and is not presented as load-bearing evidence, consistent with the small sample and the presence of the outlier W1741-46. revision: yes

Circularity Check

0 steps flagged

No significant circularity in observational comparisons

full rationale

The paper reports new JWST spectra, constructs SEDs to derive bolometric luminosities and fundamental parameters, identifies molecular species via cross-sections, and directly measures the 8-11 µm silicate feature depth and peak wavelength. It then compares these measurements to previously reported trends in the literature for inclination dependence. No equations, fitted parameters, or self-citations are used to derive or predict the reported agreement (4/5 objects) or tentative correlation; the results are empirical observations on an independent dataset with no reduction to inputs by construction.

Axiom & Free-Parameter Ledger

3 free parameters · 2 axioms · 0 invented entities

The analysis rests on standard assumptions for brown dwarf parameter estimation from spectra and SEDs, plus the premise that the sample shares a common age and that inclination angles are independently known.

free parameters (3)
  • T_eff
    Estimated from spectral features and bolometric luminosity
  • radius
    Derived from luminosity and effective temperature
  • log g
    Estimated as a fundamental parameter from mass and radius
axioms (2)
  • domain assumption The five L dwarfs are ~133 Myr members of the AB Doradus moving group and the T dwarf is ~500 Myr in the Oceanus group
    Used to establish the sample as coeval for testing inclination trends
  • domain assumption Inclination angles between ~23-90 degrees are known accurately from prior measurements
    Central to interpreting silicate absorption depth as a latitudinal effect

pith-pipeline@v0.9.0 · 5778 in / 1644 out tokens · 68749 ms · 2026-05-15T00:12:52.971708+00:00 · methodology

discussion (0)

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Works this paper leans on

103 extracted references · 103 canonical work pages · 1 internal anchor

  1. [1]

    Ackerman, A. S. & Marley, M. S. 2001, ApJ, 556, 872

  2. [2]

    2012, Philosophical Transactions of the Royal Society of London Series A, 370, 2765

    Allard, F., Homeier, D., & Freytag, B. 2012, Philosophical Transactions of the Royal Society of London Series A, 370, 2765

  3. [3]

    N., Gallimore, J

    Allers, K. N., Gallimore, J. F., Liu, M. C., & Dupuy, T. J. 2016, ApJ, 819, 133

  4. [4]

    Allers, K. N. & Liu, M. C. 2013, ApJ, 772, 79

  5. [5]

    S., et al

    Apai, D., Karalidi, T., Marley, M. S., et al. 2017, Science, 357, 683

  6. [6]

    2013, ApJ, 768, 121 Artigau, É., Bouchard, S., Doyon, R., & Lafrenière, D

    Apai, D., Radigan, J., Buenzli, E., et al. 2013, ApJ, 768, 121 Artigau, É., Bouchard, S., Doyon, R., & Lafrenière, D. 2009, ApJ, 701, 1534

  7. [7]

    2015, A&A, 577, A42 Bardalez Gagliuffi, D

    Baraffe, I., Homeier, D., Allard, F., & Chabrier, G. 2015, A&A, 577, A42 Bardalez Gagliuffi, D. C., Balmer, W. O., Pueyo, L., et al. 2025, ApJ, 988, L18 Bardalez Gagliuffi, D. C., Faherty, J. K., Li, Y ., et al. 2021, ApJ, 922, L43

  8. [8]

    2020, Resampled Opacity Database for PICASO

    Batalha, N., Freedman, R., Gharib-Nezhad, E., & Lupu, R. 2020, Resampled Opacity Database for PICASO

  9. [9]

    Best, W. M. J., Dupuy, T. J., Liu, M. C., et al. 2024, The UltracoolSheet: Photom- etry, Astrometry, Spectroscopy, and Multiplicity for 4000+Ultracool Dwarfs and Imaged Exoplanets

  10. [10]

    Best, W. M. J., Liu, M. C., Magnier, E. A., et al. 2015, ApJ, 814, 118

  11. [11]

    Best, W. M. J., Liu, M. C., Magnier, E. A., & Dupuy, T. J. 2021, AJ, 161, 42

  12. [12]

    Best, W. M. J., Sanghi, A., Liu, M. C., Magnier, E. A., & Dupuy, T. J. 2024, ApJ, 967, 115

  13. [13]

    A., V os, J

    Biller, B. A., V os, J. M., Zhou, Y ., et al. 2024, MNRAS, 532, 2207

  14. [14]

    H., Charbonneau, D., & White, R

    Blake, C. H., Charbonneau, D., & White, R. J. 2010, ApJ, 723, 684

  15. [15]

    J., Kenworthy, M

    Bohn, A. J., Kenworthy, M. A., Ginski, C., et al. 2020, ApJ, 898, L16

  16. [16]

    P., Zhou, Y ., Morley, C

    Bowler, B. P., Zhou, Y ., Morley, C. V ., et al. 2020, ApJ, 893, L30

  17. [17]

    M., Brandt, T

    Brandt, G. M., Brandt, T. D., Dupuy, T. J., Michalik, D., & Marleau, G.-D. 2021, ApJ, 915, L16

  18. [18]

    J., Kirkpatrick, J

    Burgasser, A. J., Kirkpatrick, J. D., Brown, M. E., et al. 2002, ApJ, 564, 421

  19. [19]

    K., Gonzales, E

    Burningham, B., Faherty, J. K., Gonzales, E. C., et al. 2021, MNRAS, 506, 1944

  20. [20]

    S., Line, M

    Burningham, B., Marley, M. S., Line, M. R., et al. 2017, MNRAS, 470, 1177

  21. [21]

    B., Lunine, J

    Burrows, A., Hubbard, W. B., Lunine, J. I., & Liebert, J. 2001, Reviews of Mod- ern Physics, 73, 719

  22. [22]

    2006, ApJ, 640, 1063

    Burrows, A., Sudarsky, D., & Hubeny, I. 2006, ApJ, 640, 1063

  23. [23]

    2024, JWST Calibration Pipeline

    Bushouse, H., Eisenhamer, J., Dencheva, N., et al. 2024, JWST Calibration Pipeline

  24. [24]

    A., Clayton, G

    Cardelli, J. A., Clayton, G. C., & Mathis, J. S. 1989, ApJ, 345, 245

  25. [25]

    Carnall, A. C. 2017, arXiv e-prints, arXiv:1705.05165

  26. [26]

    2023, A&A, 671, A119

    Chabrier, G., Baraffe, I., Phillips, M., & Debras, F. 2023, A&A, 671, A119

  27. [27]

    A., Tan, X., et al

    Chen, X., Biller, B. A., Tan, X., et al. 2025, MNRAS, 539, 3758

  28. [28]

    L., Kirkpatrick, J

    Cruz, K. L., Kirkpatrick, J. D., & Burgasser, A. J. 2009, AJ, 137, 3345

  29. [29]

    L., Núñez, A., Burgasser, A

    Cruz, K. L., Núñez, A., Burgasser, A. J., et al. 2018, AJ, 155, 34

  30. [30]

    C., Roellig, T

    Cushing, M. C., Roellig, T. L., Marley, M. S., et al. 2006, ApJ, 648, 614

  31. [31]

    C., Harris, H

    Dahn, C. C., Harris, H. C., Vrba, F. J., et al. 2002, AJ, 124, 1170

  32. [32]

    J., Liu, M

    Dupuy, T. J., Liu, M. C., Evans, E. L., et al. 2023, MNRAS, 519, 1688

  33. [33]

    J., Liu, M

    Dupuy, T. J., Liu, M. C., Magnier, E. A., et al. 2020, Research Notes of the American Astronomical Society, 4, 54

  34. [34]

    K., Rice, E

    Faherty, J. K., Rice, E. L., Cruz, K. L., Mamajek, E. E., & Núñez, A. 2013, AJ, 145, 2

  35. [35]

    K., Riedel, A

    Faherty, J. K., Riedel, A. R., Cruz, K. L., et al. 2016, ApJS, 225, 10

  36. [36]

    C., Rice, E

    Filippazzo, J. C., Rice, E. L., Faherty, J., et al. 2015, ApJ, 810, 158

  37. [37]

    & Apai, D

    Fuda, N. & Apai, D. 2024, ApJ, 975, L32

  38. [38]

    2024, ApJ, 965, 182 Gagné, J., Faherty, J

    Fuda, N., Apai, D., Nardiello, D., et al. 2024, ApJ, 965, 182 Gagné, J., Faherty, J. K., Cruz, K. L., et al. 2015, ApJS, 219, 33 Gagné, J., Fontaine, G., Simon, A., & Faherty, J. K. 2018a, ApJ, 861, L13 Gagné, J., Mamajek, E. E., Malo, L., et al. 2018b, ApJ, 856, 23 Gagné, J., Moranta, L., Faherty, J. K., et al. 2026, arXiv e-prints, arXiv:2602.15695 Gagn...

  39. [39]

    R., Moran, S

    Gao, P., Wakeford, H. R., Moran, S. E., & Parmentier, V . 2021, Journal of Geo- physical Research (Planets), 126, e06655

  40. [40]

    Gauza, B., Béjar, V . J. S., Pérez-Garrido, A., et al. 2015, ApJ, 804, 96

  41. [41]

    N., et al

    Ge, H., Zhang, X., Fletcher, L. N., et al. 2019, AJ, 157, 89

  42. [42]

    E., Allers, K

    Gizis, J. E., Allers, K. N., Liu, M. C., et al. 2015, ApJ, 799, 203

  43. [43]

    E., Faherty, J

    Gizis, J. E., Faherty, J. K., Liu, M. C., et al. 2012, AJ, 144, 94

  44. [44]

    K., Wakeford, H

    Grant, D., Lewis, N. K., Wakeford, H. R., et al. 2023, ApJ, 956, L32

  45. [45]

    Hoch, K. K. W., Rowland, M., Petrus, S., et al. 2025, Nature, 643, 938

  46. [46]

    J., Theissen, C

    Hsu, C.-C., Burgasser, A. J., Theissen, C. A., et al. 2021, ApJS, 257, 45

  47. [47]

    A., Liu, M

    Hurt, S. A., Liu, M. C., Zhang, Z., et al. 2024, ApJ, 961, 121

  48. [48]

    2022, A&A, 661, A80

    Jakobsen, P., Ferruit, P., Alves de Oliveira, C., et al. 2022, A&A, 661, A80

  49. [49]

    2024, igrins/plp

    Kaplan, K., Lee, J.-J., Sawczynec, E., & Kim, H.-J. 2024, igrins/plp

  50. [50]

    R., Delfosse, X., Martín, E

    Kendall, T. R., Delfosse, X., Martín, E. L., & Forveille, T. 2004, A&A, 416, L17

  51. [51]

    Kirkpatrick, J. D. 2005, ARA&A, 43, 195

  52. [52]

    D., Cruz, K

    Kirkpatrick, J. D., Cruz, K. L., Barman, T. S., et al. 2008, ApJ, 689, 1295

  53. [53]

    D., Gelino, C

    Kirkpatrick, J. D., Gelino, C. R., Faherty, J. K., et al. 2021, ApJS, 253, 7

  54. [54]

    D., Reid, I

    Kirkpatrick, J. D., Reid, I. N., Liebert, J., et al. 2000, AJ, 120, 447

  55. [55]

    R., Leggett, S

    Knapp, G. R., Leggett, S. K., Fan, X., et al. 2004, AJ, 127, 3553

  56. [56]

    Kumar, S. S. 1963, ApJ, 137, 1121

  57. [57]

    W., & Schlegel, D

    Lang, D., Hogg, D. W., & Schlegel, D. J. 2016, AJ, 151, 36

  58. [58]

    J., Almaini, O., et al

    Lawrence, A., Warren, S. J., Almaini, O., et al. 2007, MNRAS, 379, 1599

  59. [59]

    Lew, B. W. P., Apai, D., Zhou, Y ., et al. 2016, ApJ, 829, L32

  60. [60]

    C., Dupuy, T

    Liu, M. C., Dupuy, T. J., & Allers, K. N. 2016, ApJ, 833, 96

  61. [61]

    C., Magnier, E

    Liu, M. C., Magnier, E. A., Deacon, N. R., et al. 2013, ApJ, 777, L20

  62. [62]

    & Fegley, B

    Lodders, K. & Fegley, B. 2002, Icarus, 155, 393

  63. [63]

    & Fegley, Jr., B

    Lodders, K. & Fegley, Jr., B. 2006, in Astrophysics Update 2, ed. J. W. Mason, 1

  64. [64]

    Luhman, K. L. 2013, ApJ, 767, L1 Article number, page 17 of 19 A&A proofs:manuscript no. aa58421-25

  65. [65]

    Luhman, K. L. 2014, ApJ, 786, L18

  66. [66]

    Luna, J. L. & Morley, C. V . 2021, ApJ, 920, 146

  67. [67]

    T., et al

    Mace, G., Kim, H., Jaffe, D. T., et al. 2016, in Society of Photo-Optical Instru- mentation Engineers (SPIE) Conference Series, V ol. 9908, Ground-based and Airborne Instrumentation for Astronomy VI, ed. C. J. Evans, L. Simard, & H. Takami, 99080C

  68. [68]

    2018, in Society of Photo-Optical Instru- mentation Engineers (SPIE) Conference Series, V ol

    Mace, G., Sokal, K., Lee, J.-J., et al. 2018, in Society of Photo-Optical Instru- mentation Engineers (SPIE) Conference Series, V ol. 10702, Ground-based and Airborne Instrumentation for Astronomy VII, ed. C. J. Evans, L. Simard, & H. Takami, 107020Q

  69. [69]

    N., Kirkpatrick, J

    Mace, G. N., Kirkpatrick, J. D., Cushing, M. C., et al. 2013, ApJS, 205, 6

  70. [70]

    J., et al

    Mader, E., Zhang, Z., Fortney, J. J., et al. 2026, AJ, 171, 198

  71. [71]

    S., Saumon, D., Cushing, M., et al

    Marley, M. S., Saumon, D., Cushing, M., et al. 2012, ApJ, 754, 135

  72. [72]

    S., Saumon, D., & Goldblatt, C

    Marley, M. S., Saumon, D., & Goldblatt, C. 2010, ApJ, 723, L117

  73. [73]

    S., Seager, S., Saumon, D., et al

    Marley, M. S., Seager, S., Saumon, D., et al. 2002, ApJ, 568, 335

  74. [74]

    2008, Science, 322, 1348

    Marois, C., Macintosh, B., Barman, T., et al. 2008, Science, 322, 1348

  75. [75]

    M., Macintosh, B., & Barman, T

    Marois, C., Zuckerman, B., Konopacky, Q. M., Macintosh, B., & Barman, T. 2010, Nature, 468, 1080

  76. [76]

    C., Carter, A

    Matthews, E. C., Carter, A. L., Pathak, P., et al. 2024, Nature, 633, 789

  77. [77]

    G., Banerji, M., Gonzalez, E., et al

    McMahon, R. G., Banerji, M., Gonzalez, E., et al. 2013, The Messenger, 154, 35

  78. [78]

    E., Biller, B

    Miles, B. E., Biller, B. A., Patapis, P., et al. 2023, ApJ, 946, L6 Mollière, P., Kühnle, H., Matthews, E. C., et al. 2025, A&A, 703, A79 Morales-Calderón, M., Stauffer, J. R., Kirkpatrick, J. D., et al. 2006, ApJ, 653, 1454

  79. [79]

    V ., Mukherjee, S., Marley, M

    Morley, C. V ., Mukherjee, S., Marley, M. S., et al. 2024, ApJ, 975, 59

  80. [80]

    M., et al

    Nasedkin, E., Schrader, M., V os, J. M., et al. 2025, A&A, 702, A1

Showing first 80 references.