Why circumstellar disks are so faint in scattered light: The case of HD 100546

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Abstract

Context. Scattered light images of circumstellar disks play an important role in characterizing the planet forming environments around young stars. The characteristic size of the scattering dust grains can be estimated from the observed brightness asymmetry between the near and far side of the disk, for example using standard Mie theory. Such models, however, often overpredict the brightness of the disk by one or two orders of magnitude, and have difficulty explaining very red disk colors. Aims. We aim to develop a dust model that simultaneously explains the observed disk surface brightness, colors, and asymmetry in scattered light, focusing on constraining grain sizes. Methods. We use the 2D radiative transfer code MCMax with anisotropic scattering to explore the effects of grain size on synthetic scattered light images of circumstellar disks. We compare the results with surface brightness profiles of the protoplanetary disk HD 100546 in scattered light at wavelengths from 0.4 to 2.2 microns. Results. We find that extreme forward scattering by micron-sized particles lowers the effective dust albedo and creates a faint, red disk that appears only slightly forward scattering. For the outer (3;100 AU) disk of HD 100546 we derive a minimum grain size of 2.5 microns, likely present in the form of aggregates. Intermediate-sized grains are too bright, whereas smaller grains are faint and scatter more isotropically, but also produce disk colors that are too blue. Conclusions. Observed surface brightness asymmetries alone are not sufficient to constrain the grain size in circumstellar disks. Additional information, such as the brightness and colors of the disk, are needed to provide additional constraints. © 2013 ESO.

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Mulders, G. D., Min, M., Dominik, C., Debes, J. H., & Schneider, G. (2013). Why circumstellar disks are so faint in scattered light: The case of HD 100546. Astronomy and Astrophysics, 549. https://doi.org/10.1051/0004-6361/201219522

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