2024A&A...688A..42O


Query : 2024A&A...688A..42O

2024A&A...688A..42O - Astronomy and Astrophysics, volume 688A42 (2024/8-1)

The near-infrared degree of polarization in debris disks Toward a self-consistent approach to model scattered light observations.

OLOFSSON J., THEBAULT P., BAYO A., HENNING T. and MILLI J.

Abstract (from CDS):

Context. Debris disks provide a unique opportunity to probe the properties of small μm-sized particles, allowing us to peer into the constituents of their parent bodies, namely the young analogs of comets and the asteroids of our Solar System.
Aims. In the past, studies of the total intensity phase function - that is, the brightness of the disk as a function of the scattering angle - have proven powerful in constraining the main characteristics of the dust particles in debris disks. Nonetheless, there can remain some degeneracies in the modeling, which can be alleviated when considering polarized intensity observations.
Methods. We obtained new near-infrared scattered-light observations of four young debris disks, and used state-of-the-art algorithms to recover the total intensity and linear polarimetric images of the disks. These images allow us to constrain the degree of linear polarization as a function of the scattering angle.
Results. All four debris disks are detected in polarized intensity, and three are also recovered in total intensity. We measured a peak degree of polarization of ≲40% for all three disks. For the disk around HD 129590, we are also able to determine the degree of polarization in the radiation-pressure-driven halo. To reproduce the observed polarization fractions, we find that the particles must consist of highly refractive and absorbing material. For HD 129590, by measuring the polarization fraction beyond the birth ring, we constrain the width of the size distribution to be increasingly small toward greater radii, which is compatible with the effect of radiation pressure. We put these findings to the test and present a self-consistent approach to producing synthetic images, assuming different profiles for the radiation pressure strength, and accounting for the presence of unbound grains. We find the contribution of these grains to be especially critical in order to reproduce the increasing degree of polarization with stellocentric distance.
Conclusions. Some of our results - namely a very small blow-out size and very large (n, k) values for the optical constants, which are required to reproduce the observed degree of polarization - might seem difficult to reconcile with our understanding of cosmic dust. Similar results have been obtained for other disks and we discuss the current limitation of available light-scattering models as well as possible avenues to alleviate these limitations.

Abstract Copyright: © The Authors 2024

Journal keyword(s): instrumentation: high angular resolution - instrumentation: polarimeters - Kuiper belt: general - zodiacal dust - circumstellar matter

VizieR on-line data: <Available at CDS (J/A+A/688/A42): list.dat fits/*>

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 11560 * 01 53 14.6239522272 -15 10 57.400646556   9.573 9.584     A9V 9 0
2 HD 15115 PM* 02 26 16.2457848552 +06 17 33.186453252   7.15 6.80   6.33 F4IV 225 0
3 HD 32297 * 05 02 27.4358754192 +07 27 39.678553260   8.32 8.14     A0V 234 0
4 HD 35841 * 05 26 36.5868254712 -22 29 23.735043744   9.37 8.90     F3V 54 0
5 * bet Pic PM* 05 47 17.0876901 -51 03 59.441135 4.13 4.03 3.86 3.74 3.58 A6V 2087 1
6 V* CE Ant TT* 10 42 30.1018928760 -33 40 16.229805204   12.21 10.91   9.10 M2Ve 252 1
7 HD 109573 TT* 12 36 01.0317461592 -39 52 10.220465388   5.786 5.774   5.81 A0V 684 1
8 HD 111520 Or* 12 50 19.7183455512 -49 51 48.961948068   9.37 8.87     F5/6V 77 0
9 HD 114082 * 13 09 16.1926316904 -60 18 30.055543200   8.64 8.21     F3V 104 1
10 HD 115600 * 13 19 19.5409822176 -59 28 20.441034660   8.59 8.22     F2IV/V 87 1
11 HD 117255 SB* 13 30 27.7767246552 -59 24 21.397732632   9.11 8.72     F0IV/V 19 0
12 HD 129280 PM* 14 42 56.3391182520 -40 37 35.023129140   10.27 9.45     G8/K0V 15 0
13 HD 129590 * 14 44 30.9625895592 -39 59 20.628246480   9.96 9.33     G3V 73 0
14 HD 146897 Ro* 16 19 29.2418869104 -21 24 13.272759216   9.58 9.11     F2/3V 115 0
15 HD 157587 * 17 24 52.2398598216 -18 51 33.189129828   8.96 8.50     F5V 46 0
16 HD 157857 Em* 17 26 17.3317676808 -10 59 34.785507480 7.16 7.95 7.78     O6.5II(f) 181 0
17 HD 158018 * 17 27 34.6866472848 -18 20 41.704186776   9.12 8.69     F3/5V 11 0
18 HD 181327 PM* 19 22 58.9437222504 -54 32 16.975668624   7.50 7.04   6.49 F6V 331 0
19 HD 191089 SB? 20 09 05.2156358688 -26 13 26.520165768   7.62 7.18     F5V 177 0
20 HD 191131 * 20 09 20.3727266640 -27 57 20.349897264   8.80 8.46     F0V 28 0
21 HD 197481 BY* 20 45 09.5324974119 -31 20 27.237889841   10.05 8.627 9.078 6.593 M1VeBa1 1344 0

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