Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/7615
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dc.contributor.authorMillar-Blanchaer, M. A-
dc.contributor.authorGirard, J. H-
dc.contributor.authorKaralidi, T-
dc.contributor.authorMarley, M. S-
dc.contributor.authorvan Holstein, R. G-
dc.contributor.authorSengupta, S-
dc.contributor.authorMawet, Dimitri-
dc.contributor.authorKataria, Tiffany-
dc.contributor.authorJos de Boer, F. S-
dc.date.accessioned2021-02-07T06:19:15Z-
dc.date.available2021-02-07T06:19:15Z-
dc.date.issued2020-05-01-
dc.identifier.citationThe Astrophysical Journal, Vol. 894, No. 1, 42en_US
dc.identifier.issn0004-637X-
dc.identifier.urihttp://hdl.handle.net/2248/7615-
dc.descriptionRestricted Accessen_US
dc.description.abstractBrown dwarfs exhibit patchy or spatially varying banded cloud structures that are inferred through photometric and spectroscopic variability modeling techniques. However, these methods are insensitive to rotationally invariant structures, such as the bands seen in Jupiter. Here, we present H-band Very Large Telescope/NaCo linear polarization measurements of the nearby Luhman 16 L/T transition binary, which suggest that Luhman 16A exhibits constant longitudinal cloud bands. The instrument was operated in pupil tracking mode, allowing us to unambiguously distinguish between a small astrophysical Brown dwarfs exhibit patchy or spatially varying banded cloud structures that are inferred through photometric and spectroscopic variability modeling techniques. However, these methods are insensitive to rotationally invariant structures, such as the bands seen in Jupiter. Here, we present H-band Very Large Telescope/NaCo linear polarization measurements of the nearby Luhman 16 L/T transition binary, which suggest that Luhman 16A exhibits constant longitudinal cloud bands. The instrument was operated in pupil tracking mode, allowing us to unambiguously distinguish between a small astrophysical polarization and the ∼2% instrumental linear polarization. We measure the degree and angle of linear polarization of Luhman 16A and B to be pA = 0.031% ± 0.004% and ψA = −32° ± 4°, and pB = 0.010% ± 0.004% and y b= 73 +13 -11 13 , respectively. Using known physical parameters of the system, we demonstrate that an oblate homogeneous atmosphere cannot account for the polarization measured in Luhman 16A, but could be responsible for that of the B component. Through a nonexhaustive search of banded cloud morphologies, we demonstrate a two-banded scenario that can achieve a degree of linear polarization of p = 0.03% and conclude that the measured polarization of the A component must be predominantly due to cloud banding. For Luhman 16B, either oblateness or cloud banding could be the dominant source of the measured polarization. The misaligned polarization angles of the two binary components tentatively suggest spin–orbit misalignment. These measurements provide new evidence for the prevalence of cloud banding in brown dwarfs while at the same time demonstrating a new method—complementary to photometric and spectroscopic variability methods—for characterizing the cloud morphologies of substellar objects without signs of variability.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.relation.urihttps://doi.org/10.3847/1538-4357/ab6ef2-
dc.rights© The American Astronomical Society-
dc.subjectNear infrared astronomyen_US
dc.subjectVery Large Telescopeen_US
dc.subjectPolarimetryen_US
dc.titleDetection of Polarization due to Cloud Bands in the Nearby Luhman 16 Brown Dwarf Binaryen_US
dc.typeArticleen_US
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