REVIEW 3 major objections 6 minor 63 references
Spectroscopy of Free-Floating Planetary-Mass Objects and their disks with JWST
T0 review · 3 major / 6 minor · reviewed 2026-08-06 · deepseek-v4-flash
Pith's one-line read Six of eight free-floating planetary-mass objects observed with JWST show mid-infrared silicate emission from disks, and one shows photospheric silicate absorption, evidence that disks and atmospheres of these 5-10 Jupiter-mass objects…
desk verdict First JWST 1-13 µm spectral survey of free-floating planetary-mass objects: the disk excess detections are solid, but the two headline 'firsts' (photospheric silicate absorption and grain growth) rest on an extinction law the authors admit is only an average. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The argument is carried by the 10 µm silicate feature and its relation to the photospheric model spectrum. A silicate emission or absorption feature arises from the stretching vibration of Si-O bonds in warm dust; its shape and strength are read through continuum-normalized spectra, a flux ratio at 11.3 vs 9.8 µm, and a silicate index, the ratio of continuum flux to absorption flux at 9.0 µm. The paper dereddens every MIRI spectrum with the Gordon et al. (2023) extinction law and compares the derived feature parameters with published brown dwarf, T Tauri, and Herbig Ae/Be samples. This lets the authors separate an amorphous, interstellar-like dust signature, a single 9-10 µm peak, from processed, crystalline-rich dust with additional peaks near 9.3 and 11.3 µm, and to attach photospheric absorption, rather than disk emission, to cloud-bearing atmospheres.
What would settle it
Re-observe UGC0417+2832 with the MIRI medium-resolution spectrometer, deredden using a sightline-specific extinction curve measured from nearby stars along the same line of sight, and re-measure the 9.0 µm silicate index; if the index becomes consistent with unity under that correction, the photospheric silicate absorption is an artifact of the adopted extinction. Alternatively, a larger sample of young diskless free-floating planetary-mass objects with independently measured extinctions could show whether silicate absorption strength tracks spectral type as it does for brown dwarfs.
Extended reading notes
Core claim
On the paper's own terms, the central discovery is that disks around free-floating planetary-mass objects are not merely present but actively evolving: six of eight targets show mid-infrared excess with 10 µm silicate emission features whose shapes and strengths indicate grain growth and crystallization, comparable to more massive brown dwarfs and stars. In addition, one disk-free target, UGC0417+2832, shows a 10 µm silicate absorption feature in its photosphere, the first such detection in a very young free-floating planetary-mass object, interpreted as silicate clouds in a cool 1600 K atmosphere. The paper also finds methane and ethylene emission lines in several of the disks and notes photospheric diversity in the 3-5 µm region that current atmospheric models do not reproduce. Together these observations make the eight objects the lowest-mass isolated objects in which disk silicate and hydrocarbon emission have been seen.
Load-bearing premise
The silicate feature shapes and the photospheric absorption claim rest on dereddening every spectrum with extinction values from near-infrared template fits and with one average Milky Way extinction law; if the true extinction toward UGC0417+2832, or the 10 µm extinction curve along that sightline, differs substantially, the silicate absorption detection could weaken or vanish.
Editorial extensions
If this is right
- Disks around 5-10 Jupiter-mass free-floating objects undergo the same dust-processing sequence, grain growth and crystallization, seen in disks around stars and brown dwarfs, so planet formation conditions are not unique to higher-mass hosts.
- The 10 µm silicate absorption in UGC0417+2832, if real, shows that silicate clouds can form in very young planetary-mass atmospheres at about 1600 K, not only in older field brown dwarfs.
- Hydrocarbon emission, methane at 7.7 µm and ethylene at 10.5 µm, in several disks indicates carbon-rich inner-disk chemistry can arise around planetary-mass objects, as in low-mass stars.
- The presence and evolutionary state of these disks imply the potential for rocky companions to form around free-floating planetary-mass objects.
- The unexplained 3-5 µm photospheric diversity means current atmospheric models miss a parameter, possibly cloud distribution, metallicity, or inclination-dependent cloud opacity, that shapes these spectra at similar temperatures.
Reading between the lines
- Editorial extension: if silicate emission features are common in this mass range, mid-infrared spectroscopy of larger samples of free-floating planetary-mass objects could become a statistical probe of disk evolution and dust processing across star-forming regions.
- The paper's own caveat about dereddening implies the photospheric silicate absorption claim should be tested with a sightline-specific extinction measurement, for example higher-resolution MIRI/MRS spectroscopy of UGC0417+2832 and neighbouring stars.
- The two objects without disks were selected on the basis of IRAC excess, so the 6-in-8 disk fraction here is not an unbiased census; an unbiased survey could confirm or revise the apparent disk fraction among planetary-mass objects.
- If silicate clouds form at 1600 K in young objects, the same 10 µm absorption search in other young, diskless free-floating planetary-mass objects could map cloud formation as a function of spectral type and age, extending the brown-dwarf silicate-index sequence.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This manuscript presents JWST NIRSpec (1-5 um) and MIRI LRS (5-13 um) spectra of eight free-floating planetary-mass objects (FFPMOs) in Taurus, Chamaeleon I, and rho Ophiuchus. The authors derive spectral types M9.5-L4, effective temperatures 1600-1900 K, extinctions A_V = 1.3-7 mag, and masses below 0.01 M_sun from an HR diagram. Six of eight objects show mid-infrared excess above the best-fit BT-Settl photospheric model and 10 um silicate emission; the shapes are used to infer grain growth and crystallization. One object without a disk, UGC0417+2832, is reported to show photospheric silicate absorption, claimed as a first for very young FFPMOs. Several objects show hydrocarbon emission lines attributed to disks. The paper concludes that disks around planetary-mass objects undergo dust processing similar to brown dwarfs and stars.
Significance. The dataset is valuable: it is the first systematic 1-13 um spectroscopic survey of FFPMOs with JWST, and the presence of mid-infrared excess is directly visible in the observed spectra (Figures 2 and 5) without recourse to the dereddening procedure, making the disk detections robust. If the extinction-law systematics are properly quantified, the silicate emission and absorption results would constitute a substantial advance in understanding disk evolution and cool atmospheres at planetary masses. The authors are appropriately cautious about model-dependent temperatures and the low resolution of the molecular line identification. However, the two most distinctive claims -- the photospheric silicate absorption 'first' and the 'strong evidence of grain growth and crystallization' -- are measured on dereddened spectra and are sensitive to the adopted average extinction law, which the authors themselves note is not representative of individual sightlines. The paper does not currently propagate this systematic uncertainty into the quoted results.
major comments (3)
- [4.2] The dereddening of the MIRI spectra uses the Gordon et al. (2023) extinction law, which includes an interstellar silicate absorption feature near 9.7 um. As the paper itself states in Section 4.2, this law 'does not represent the specific line of sight extinction to the targets.' Because the silicate emission/absorption analysis in Sections 4.2 and 4.3 is performed on dereddened spectra, an error in the strength or shape of the 9.7 um extinction feature will directly create or suppress a 10 um silicate feature. The error bars in Figures 10 and 11 propagate only the +-1 mag uncertainty in A_V, not the systematic uncertainty in the extinction law. I request that the authors repeat the silicate index and the continuum-normalized shape measurements with alternative extinction laws (e.g., Fitzpatrick 1999 with a range of R_V, or regional extinction curves) and report the resulting range in the silicate index and F11.3/F9.8 ratio. Without this, the claims of photospheric silicate absorption in UGC0417+2832 and of 'strong evidence of grain growth and crystallization' are not yet robust.
- [4.3] The detection of silicate absorption in UGC0417+2832 is reported without a significance estimate. The silicate index is a ratio of continuum to absorption flux at 9.0 um, but Figure 11 does not show the uncertainty from spectral noise or the number of independent resolution elements contributing to the average. Given that this object has A_V = 4.3 mag and the dereddening correction is substantial, the authors should report a formal significance (e.g., the absorption depth in units of the noise) and show the spectrum before and after dereddening to demonstrate that the 9 um dip is not introduced by the correction. The statement in Section 4.3 that UGC0417+2832 'shows silicate in absorption' is stronger than what is currently demonstrated.
- [4.2, Figure 10] The conclusion that FFPMO disks show a higher degree of grain growth and crystallization than the comparison sample depends on the dereddening-induced shift of the six points in the F11.3/F9.8 versus peak-over-continuum plane. The comparison sample from Pascucci et al. (2009) is likely uncorrected for extinction, so the offset between the two samples is not a homogeneous comparison. The qualitative classification of the features in Figure 9 into amorphous and crystalline silicates also rests on the dereddened spectra. The claim should be softened to state that, under the adopted extinction law, the FFPMO points move into a region consistent with more processed silicates, and the systematic uncertainty in this offset should be quantified as in Comment 1.
minor comments (6)
- [Title] The title contains an erroneous space in 'F ree-Floating' (a LaTeX artifact in the manuscript text); it should read 'Free-Floating'.
- [3.1] The spectral type fitting uses the Fitzpatrick (1999) extinction law, while the model fitting and dereddening use Gordon et al. (2023); the paper states that the choice has no significant effect (citing Almendros-Abad et al. 2022), but it would be clearer to quantify this for the present sample given that the A_V values are subsequently used in the MIR dereddening.
- [Figure 1] The x-axis label 'MK - M[4.5]' is confusing because both quantities are absolute magnitudes; it should be labeled as a color (e.g., 'K - [4.5]') with a note that the distance modulus cancels.
- [4.1] The 8.0/3.6 um flux ratio is said to be extinction-corrected, but the correction method is described later in Section 4.2; adding a cross-reference would help the reader.
- [4.4] The statement that the 10.5 um feature is more plausibly ethylene is reasonable, but the lack of a quantitative comparison of the line flux with the expected hydrogen 12-8 line makes the identification tentative; this caveat should be reflected in the abstract, which currently lists hydrocarbon emission without this qualification.
- [Abstract] The sentence 'These are the lowest mass isolated objects found so far with silicate and hydrocarbon emission features arising in their disks' could be read as applying to all six disk objects, whereas hydrocarbon emission is securely reported for only four objects and tentatively for others; a more precise wording would distinguish the silicate and hydrocarbon subsets.
Circularity Check
No circularity: results are observational measurements with an acknowledged extinction-law systematic, not predictions derived from fitted inputs.
full rationale
This is an observational characterization paper rather than a derivation chain, and I find no load-bearing circular step. Spectral types and A_V are obtained by standard template and BT-Settl model fitting to the 1-2.5 micron NIRSpec data (Sections 3.1-3.2), and the mid-infrared excess, silicate emission, and silicate absorption diagnostics are then measured on the dereddened MIRI spectra (Sections 4.1-4.3). No result claimed as a 'prediction' is constructed from the fitted parameters: the silicate indices are direct flux ratios with independent local continuum fits. The main vulnerability is the assumed extinction law: the paper dereddens with Gordon et al. (2023) and explicitly cautions that 'the extinction law does not represent the specific line of sight extinction to the targets' and that 'differences in the extinction laws may alter the shape of the silicate feature' (Section 4.2). That is a correctly stated systematic uncertainty affecting interpretation, not a circular argument, because the dereddening curve is imported from external published measurements and is not derived from the targets' own silicate features. The only overlapping-author citation, Flagg et al. (2025), provides prior hydrocarbon-line detections for CHA1107-7626; the present paper independently detects the same features in its own MIRI spectra and in three other disks (Section 4.4), so the citation is not load-bearing. The results are externally falsifiable against the published spectra and photometry. Score 0.
Assumptions & free parameters
free parameters (4)
- Effective temperature Teff =
1600-1900 K (per object)
- Surface gravity log g =
3.5 (cgs)
- Extinction Av =
1.3-7.0 mag (per object)
- Radius R =
1.8-3.8 RJup (per object)
assumptions (5)
- domain assumption Targets are members of young (1-5 Myr) star-forming regions Taurus, Chamaeleon I, and rho Ophiuchus.
- domain assumption Distances derived from Gaia DR3 parallaxes of nearby stellar members are representative for each target.
- domain assumption The Gordon et al. (2023) extinction law applies along each line of sight.
- domain assumption BT-Settl model atmospheres and ATMO-2020 evolutionary tracks are valid for these objects.
- domain assumption The 10.5 um emission line is ethylene rather than H I 12-8.
Cite this review
Pith. "Pith review of Spectroscopy of Free-Floating Planetary-Mass Objects and their disks with JWST." pith.science (2026). https://pith.science/paper/A5F4IFGN
@misc{pith2026250705155,
author = {Pith},
title = {Pith review of: Spectroscopy of Free-Floating Planetary-Mass Objects and their disks with JWST},
year = {2026},
howpublished = {\url{https://pith.science/paper/A5F4IFGN}},
note = {Machine review of arXiv:2507.05155}
}
abstract
Free-floating planetary-mass objects (FFPMOs) are known to harbor disks at young ages. Here, we present 1-13 $\mu m$ spectra for eight young FFPMOs with masses of 5-10 M$_\mathrm{Jup}$ (at ages of 1-5 Myr), using the NIRSpec and MIRI instruments on the James Webb Space Telescope. We derive fundamental properties of these targets, and find spectral types of M9.5 to L4, with effective temperatures of 1600-1900 K. The photospheric spectra of our targets show a clear diversity at similar temperatures, especially in the 3-5 $\mu m$ range, unaccounted for by existing atmospheric models. We find a silicate absorption feature in the photosphere of one of our targets, the first such detection in very young FFPMOs, indicating silicate clouds in their cool atmospheres. Six of our objects show mid-infrared excess emission above the photosphere, as well as silicate emission features, demonstrating the presence of disks. The shape and strength of the latter features constitute strong evidence of grain growth and crystallization, similar to what is seen in more massive brown dwarfs and stars. We also detect emission lines from hydrocarbon molecules in the disks of several targets. These are the lowest mass isolated objects found so far with silicate and hydrocarbon emission features arising in their disks. The presence of disks and their characteristics point to the potential for the formation of rocky companions around free-floating planetary-mass objects.
Figures
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Reference graph
Works this paper leans on
-
[1]
Allard, F., Homeier, D., & Freytag, B. 2012, Philosophical Transactions of the Royal Society of London Series A, 370, 2765, doi: 10.1098/rsta.2011.0269
arXiv 2012
-
[2]
Allers, K. N., & Liu, M. C. 2013, ApJ, 772, 79, doi: 10.1088/0004-637X/772/2/79 —. 2020, PASP, 132, 104401, doi: 10.1088/1538-3873/aba811
-
[3]
2022, A&A, 657, A129, doi: 10.1051/0004-6361/202142050
Krone-Martins, A., & Kubiak, K. 2022, A&A, 657, A129, doi: 10.1051/0004-6361/202142050
-
[4]
2005, Science, 310, 834, doi: 10.1126/science.1118042
Apai, D., Pascucci, I., Bouwman, J., et al. 2005, Science, 310, 834, doi: 10.1126/science.1118042
-
[5]
M., Kamp, I., Henning, T., et al
Arabhavi, A. M., Kamp, I., Henning, T., et al. 2024, Science, 384, 1086, doi: 10.1126/science.adi8147 —. 2025, arXiv e-prints, arXiv:2506.02748. https://arxiv.org/abs/2506.02748 Astropy Collaboration, Robitaille, T. P., Tollerud, E. J., et al. 2013, A&A, 558, A33, doi: 10.1051/0004-6361/201322068 Astropy Collaboration, Price-Whelan, A. M., Sip˝ ocz, B. M....
arXiv 2024
-
[6]
2021, AJ, 161, 147, doi: 10.3847/1538-3881/abd806
Demleitner, M., & Andrae, R. 2021, AJ, 161, 147, doi: 10.3847/1538-3881/abd806
-
[7]
2015, A&A, 577, A42, doi: 10.1051/0004-6361/201425481
Baraffe, I., Homeier, D., Allard, F., & Chabrier, G. 2015, A&A, 577, A42, doi: 10.1051/0004-6361/201425481
-
[8]
2017, ApJL, 841, L11, doi: 10.3847/2041-8213/aa7046
Bayo, A., Joergens, V., Liu, Y., et al. 2017, ApJL, 841, L11, doi: 10.3847/2041-8213/aa7046
Show all 63 references
-
[9]
J., Esposito, V
Boersma, C., Allamandola, L. J., Esposito, V. J., et al. 2023, ApJ, 959, 74, doi: 10.3847/1538-4357/ad022b
2023 doi
-
[10]
Burgasser, A. J. 2014, in Astronomical Society of India Conference Series, Vol. 11, Astronomical Society of India Conference Series, 7–16. https://arxiv.org/abs/1406.4887
2014 arXiv
-
[11]
2024, JWST Calibration Pipeline, 1.15.1, Zenodo, doi: 10.5281/zenodo.12692459
Bushouse, H., Eisenhamer, J., Dencheva, N., et al. 2024, JWST Calibration Pipeline, 1.15.1, Zenodo, doi: 10.5281/zenodo.12692459
2024 doi
-
[12]
L., Stapelfeldt, K
Cieza, L., Padgett, D. L., Stapelfeldt, K. R., et al. 2007, ApJ, 667, 308, doi: 10.1086/520698
2007 doi
-
[13]
L., N´ u˜ nez, A., Burgasser, A
Cruz, K. L., N´ u˜ nez, A., Burgasser, A. J., et al. 2018, AJ, 155, 34, doi: 10.3847/1538-3881/aa9d8a
2018 doi
-
[14]
C., Roellig, T
Cushing, M. C., Roellig, T. L., Marley, M. S., et al. 2006, ApJ, 648, 614, doi: 10.1086/505637
2006 doi
-
[15]
Damian, B., Jose, J., Biller, B., & Paul, K. T. 2023a, Journal of Astrophysics and Astronomy, 44, 77, doi: 10.1007/s12036-023-09968-2
-
[16]
2023b, ApJ, 951, 139, doi: 10.3847/1538-4357/acd115
Damian, B., Jose, J., Biller, B., et al. 2023b, ApJ, 951, 139, doi: 10.3847/1538-4357/acd115
-
[17]
D., Andrews, J
Decleir, M., Gordon, K. D., Andrews, J. E., et al. 2022, ApJ, 930, 15, doi: 10.3847/1538-4357/ac5dbe
2022 doi
-
[18]
2012, A&A, 548, A26, doi: 10.1051/0004-6361/201219984 14 Damian et al
Delorme, P., Gagn´ e, J., Malo, L., et al. 2012, A&A, 548, A26, doi: 10.1051/0004-6361/201219984 14 Damian et al
2012 doi
-
[19]
J., Liu, M
Dupuy, T. J., Liu, M. C., Evans, E. L., et al. 2023, MNRAS, 519, 1688, doi: 10.1093/mnras/stac3557
2023 doi
-
[20]
J., Liu, M
Dupuy, T. J., Liu, M. C., Magnier, E. A., et al. 2020, Research Notes of the American Astronomical Society, 4, 54, doi: 10.3847/2515-5172/ab8942
2020 doi
-
[21]
L., & Luhman, K
Esplin, T. L., & Luhman, K. L. 2019, AJ, 158, 54, doi: 10.3847/1538-3881/ab2594 —. 2020, AJ, 159, 282, doi: 10.3847/1538-3881/ab8dbd
2019 doi
-
[22]
L., Luhman, K
Esplin, T. L., Luhman, K. L., Faherty, J. K., Mamajek, E. E., & Bochanski, J. J. 2017, AJ, 154, 46, doi: 10.3847/1538-3881/aa74e2
2017 doi
-
[23]
Fitzpatrick, E. L. 1999, PASP, 111, 63, doi: 10.1086/316293
1999 doi
- [24]
-
[25]
2024, A&A, 687, A96, doi: 10.1051/0004-6361/202348034 Gagn´ e, J., Faherty, J
Franceschi, R., Henning, T., Tabone, B., et al. 2024, A&A, 687, A96, doi: 10.1051/0004-6361/202348034 Gagn´ e, J., Faherty, J. K., Cruz, K. L., et al. 2015, ApJS, 219, 33, doi: 10.1088/0067-0049/219/2/33 Gaia Collaboration, Prusti, T., de Bruijne, J. H. J., et al. 2016, A&A, 5...
2024 doi
-
[26]
D., Cartledge, S., & Clayton, G
Gordon, K. D., Cartledge, S., & Clayton, G. C. 2009, ApJ, 705, 1320, doi: 10.1088/0004-637X/705/2/1320
2009 doi
-
[27]
D., Clayton, G
Gordon, K. D., Clayton, G. C., Decleir, M., et al. 2023, ApJ, 950, 86, doi: 10.3847/1538-4357/accb59
2023 doi
-
[28]
D., Misselt, K
Gordon, K. D., Misselt, K. A., Bouwman, J., et al. 2021, ApJ, 916, 33, doi: 10.3847/1538-4357/ac00b7
2021 doi
-
[29]
A., Liu, M
Hurt, S. A., Liu, M. C., Zhang, Z., et al. 2024, ApJ, 961, 121, doi: 10.3847/1538-4357/ad0b12
2024 doi
-
[30]
R., Stelzer, B., & Haisch, Jr., K
Jayawardhana, R., Ardila, D. R., Stelzer, B., & Haisch, Jr., K. E. 2003, AJ, 126, 1515, doi: 10.1086/377144
2003 doi
-
[31]
Jayawardhana, R., & Ivanov, V. D. 2006, Science, 313, 1279, doi: 10.1126/science.1132128
2006 doi
-
[32]
2013, A&A, 558, L7, doi: 10.1051/0004-6361/201322432 JWST Transiting Exoplanet Community Early Release Science Team, Ahrer, E.-M., Alderson, L., et al
Joergens, V., Bonnefoy, M., Liu, Y., et al. 2013, A&A, 558, L7, doi: 10.1051/0004-6361/201322432 JWST Transiting Exoplanet Community Early Release Science Team, Ahrer, E.-M., Alderson, L., et al. 2023, Nature, 614, 649, doi: 10.1038/s41586-022-05269-w
2013 doi
-
[33]
B., Scholz, A., Muˇ zi´ c, K., et al
Langeveld, A. B., Scholz, A., Muˇ zi´ c, K., et al. 2024, AJ, 168, 179, doi: 10.3847/1538-3881/ad6f0c
2024 doi
-
[34]
W., & Roche, P
Lucas, P. W., & Roche, P. F. 2000, MNRAS, 314, 858, doi: 10.1046/j.1365-8711.2000.03515.x
2000
-
[35]
Luhman, K. L. 2007, ApJS, 173, 104, doi: 10.1086/520114
2007 doi
-
[36]
L., Adame, L., D’Alessio, P., et al
Luhman, K. L., Adame, L., D’Alessio, P., et al. 2005, ApJL, 635, L93, doi: 10.1086/498868
2005 doi
-
[37]
L., & Alves de Oliveira, C
Luhman, K. L., & Alves de Oliveira, C. 2025, arXiv e-prints, arXiv:2506.08969. https://arxiv.org/abs/2506.08969
2025 arXiv
-
[38]
L., Mamajek, E
Luhman, K. L., Mamajek, E. E., Shukla, S. J., & Loutrel, N. P. 2017, AJ, 153, 46, doi: 10.3847/1538-3881/153/1/46
2017 doi
-
[39]
L., Allen, L
Luhman, K. L., Allen, L. E., Allen, P. R., et al. 2008, ApJ, 675, 1375, doi: 10.1086/527347
2008 doi
-
[40]
2024, AJ, 167, 168, doi: 10.3847/1538-3881/ad2938 Mart ´ ın, E
Manjavacas, E., Tremblin, P., Birkmann, S., et al. 2024, AJ, 167, 168, doi: 10.3847/1538-3881/ad2938 Mart ´ ın, E. L.,{ˇZ}erjal, M., Bouy, H., et al. 2024, arXiv e-prints, arXiv:2405.13497, doi: 10.48550/arXiv.2405.13497
2024 doi
-
[41]
E., Biller, B
Miles, B. E., Biller, B. A., Patapis, P., et al. 2023, ApJL, 946, L6, doi: 10.3847/2041-8213/acb04a
2023 doi
-
[42]
N., et al
Miret-Roig, N., Bouy, H., Raymond, S. N., et al. 2022, Nature Astronomy, 6, 89, doi: 10.1038/s41550-021-01513-x
2022 doi
-
[43]
2004, ApJL, 609, L33, doi: 10.1086/422555 Muˇ zi´ c, K., Scholz, A., Geers, V
Mohanty, S., Jayawardhana, R., Natta, A., et al. 2004, ApJL, 609, L33, doi: 10.1086/422555 Muˇ zi´ c, K., Scholz, A., Geers, V. C., Jayawardhana, R., & L´ opez Mart ´ ı, B. 2014, ApJ, 785, 159, doi: 10.1088/0004-637X/785/2/159
2004 doi
-
[44]
2001, A&A, 376, L22, doi: 10.1051/0004-6361:20011055
Natta, A., & Testi, L. 2001, A&A, 376, L22, doi: 10.1051/0004-6361:20011055
2001 doi
-
[45]
2009, ApJ, 696, 143, doi: 10.1088/0004-637X/696/1/143
Pascucci, I., Apai, D., Luhman, K., et al. 2009, ApJ, 696, 143, doi: 10.1088/0004-637X/696/1/143
2009 doi
-
[46]
W., Tremblin, P., Baraffe, I., et al
Phillips, M. W., Tremblin, P., Baraffe, I., et al. 2020, A&A, 637, A38, doi: 10.1051/0004-6361/201937381
2020 doi
-
[47]
2022, European Physical Journal Plus, 137, 1206, doi: 10.1140/epjp/s13360-022-03384-1
Pinilla, P. 2022, European Physical Journal Plus, 137, 1206, doi: 10.1140/epjp/s13360-022-03384-1
2022 doi
-
[48]
2024, A&A, 686, A37, doi: 10.1051/0004-6361/202347327
Piscarreta, L., Muˇ zi´ c, K., Almendros-Abad, V., & Scholz, A. 2024, A&A, 686, A37, doi: 10.1051/0004-6361/202347327
2024 doi
-
[49]
2014, ApJ, 793, 75, doi: 10.1088/0004-637X/793/2/75
Radigan, J., Lafreni` ere, D., Jayawardhana, R., & Artigau, E. 2014, ApJ, 793, 75, doi: 10.1088/0004-637X/793/2/75
2014 doi
-
[50]
2023, PASP, 135, 048001, doi: 10.1088/1538-3873/acb293
Rigby, J., Perrin, M., McElwain, M., et al. 2023, PASP, 135, 048001, doi: 10.1088/1538-3873/acb293
2023 doi
-
[51]
C., Best, W
Sanghi, A., Liu, M. C., Best, W. M. J., et al. 2023, ApJ, 959, 63, doi: 10.3847/1538-4357/acff66
2023 doi
-
[52]
C., Windsor, J., Cushing, M
Schneider, A. C., Windsor, J., Cushing, M. C., Kirkpatrick, J. D., & Wright, E. L. 2016, ApJL, 822, L1, doi: 10.3847/2041-8205/822/1/L1
2016 doi
-
[53]
2008, ApJL, 672, L49, doi: 10.1086/526340
Scholz, A., & Jayawardhana, R. 2008, ApJL, 672, L49, doi: 10.1086/526340
2008 doi
-
[54]
2012, ApJ, 756, 24, doi: 10.1088/0004-637X/756/1/24
Scholz, A., Jayawardhana, R., Muzic, K., et al. 2012, ApJ, 756, 24, doi: 10.1088/0004-637X/756/1/24
2012 doi
-
[55]
2007, ApJ, 660, 1517, doi: 10.1086/513066
Scholz, A., Jayawardhana, R., Wood, K., et al. 2007, ApJ, 660, 1517, doi: 10.1086/513066
2007 doi
-
[56]
2023, AJ, 165, 196, doi: 10.3847/1538-3881/acc65d JWST spectroscopy of planetary-mass objects 15
Scholz, A., Muzic, K., Jayawardhana, R., Almendros-Abad, V., & Wilson, I. 2023, AJ, 165, 196, doi: 10.3847/1538-3881/acc65d JWST spectroscopy of planetary-mass objects 15
2023 doi
-
[57]
2005, A&A, 430, L49, doi: 10.1051/0004-6361:200400121
Lodieu, N. 2005, A&A, 430, L49, doi: 10.1051/0004-6361:200400121
2005 doi
-
[58]
H., & Scholz, A
Seo, H. H., & Scholz, A. 2025, MNRAS, 537, 2579, doi: 10.1093/mnras/staf163
2025 doi
-
[59]
2012, ApJ, 760, 151, doi: 10.1088/0004-637X/760/2/151 Su´ arez, G., & Metchev, S
Sorahana, S., & Yamamura, I. 2012, ApJ, 760, 151, doi: 10.1088/0004-637X/760/2/151 Su´ arez, G., & Metchev, S. 2022, MNRAS, 513, 5701, doi: 10.1093/mnras/stac1205 Su´ arez, G., Vos, J. M., Metchev, S., Faherty, J. K., & Cruz, K. 2023, ApJL, 954, L6, doi: 10.3847/2041-8213/acec4b
2012 doi
-
[60]
S., Lada, C
Teixeira, P. S., Lada, C. J., Marengo, M., & Lada, E. A. 2012, A&A, 540, A83, doi: 10.1051/0004-6361/201015326
2012 doi
-
[61]
2011, ApJ, 734, 73, doi: 10.1088/0004-637X/734/2/73
Tsuji, T., Yamamura, I., & Sorahana, S. 2011, ApJ, 734, 73, doi: 10.1088/0004-637X/734/2/73
2011 doi
-
[62]
M., et al
Venuti, L., Stelzer, B., Alcal´ a, J. M., et al. 2019, A&A, 632, A46, doi: 10.1051/0004-6361/201935745
2019 doi
-
[63]
M., Allers, K
Vos, J. M., Allers, K. N., & Biller, B. A. 2017, ApJ, 842, 78, doi: 10.3847/1538-4357/aa73cf Zapatero Osorio, M. R., B´ ejar, V. J. S., Mart ´ ın, E. L., et al. 2000, Science, 290, 103, doi: 10.1126/science.290.5489.103
2017 doi
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