Table 2
NEATM best-fit parameters and other measurements of interest.
Object | S/N | Hv | R (km) | ρv | η | Rref (km) | ![]() |
ηref |
---|---|---|---|---|---|---|---|---|
10199 Chariklo | 72 | 7.00 ± 0.2 | 129.2 ± 1.1 | 0.042 ± 0.008 | 0.85 ± 0.01 | ![]() |
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118.4 ± 3.4 (b) | ![]() |
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||||||
44594 (1999 OX3) | 13 | 7.07 ± 0.2 | 54.64 ± 1.50 | 0.220 ± 0.040 | 0.66 ± 0.01 | ![]() |
![]() |
![]() |
54598 Bienor | 42 | 7.46 ± 0.2 | 75.65 ± 4.50 | 0.080 ± 0.015 | 1.37 ± 0.05 | ![]() |
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||||||
468861 (2013 LU28) | 227 | 8.29 ± 0.2 | 52.04 ± 0.12 | 0.079 ± 0.014 | 0.86 ± 0.01 | − | − | − |
2020 VF1 | 115 | 9.93 ± 0.2 | 28.51 ± 0.25 | 0.058 ± 0.011 | 0.84 ± 0.02 | − | − | − |
459865 (2013 XZ8) | 181 | 9.50 ± 0.2 | 36.53 ± 0.08 | 0.053 ± 0.010 | 0.79 ± 0.01 | − | − | − |
469442 (2002 GG166) | 8 | 8.23 ± 0.02 | 51.29 ± 5.10 | 0.08 ± 0.03 | 1.00 (fixed) | − | − | − |
Notes. The signal-to-noise ratio was estimated in the 12–25 μm range. Hv was retrieved from the IMCCE database SsODNet (Berthier et al. 2023) for all objects except for Chariklo, for which we considered Hv=7.0 ± 0.2 instead of the IMCCE value (6.54) because the magnitude of Chariklo varies in time due to its elliptical form and its rings (Braga-Ribas et al. 2014; Lellouch et al. 2017). We assumed G=0.15 for all our targets. “ref” refers to earlier measurements ((a) Lellouch et al. 2017, (b) Fornasier et al. 2013, (c) Lellouch et al. 2013, and (d) Duffard et al. 2014).
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