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Table 1

Derived diameters (D), visible geometric albedos (pV), and beaming parameters (η).

Object H G12 D(km) pV η Fit n9 n18 r (au) Δ (au) α (°) MJD
00001 3.43 0.88 1082.6 0.064 1.05 True 2 1 2.95137 2.77621 20.01867 53868.7602
00001 3.43 0.88 929.9 0.087 0.94 False 0 2 2.98621 2.82770 19.37133 54048.8055
00001 3.43 0.88 1029.9 0.071 0.96 False 1 1 2.88090 2.69998 20.59184 54324.6499
00002 4.22 0.68 556.99 0.117 1.00 True 3 3 3.38096 3.23953 17.24352 54006.1010
00002 4.22 0.68 535.46 0.126 0.99 True 3 3 3.34383 3.18900 17.66837 54259.5766
00003 5.19 0.18 268.28 0.206 1.14 True 3 2 2.96530 2.79400 19.37168 54116.1894
00003 5.19 0.18 247.44 0.242 1.08 True 1 2 3.25764 3.10484 18.18754 54288.8980
00004 2.99 0.36 562.61 0.355 1.10 True 2 3 2.18592 1.95199 26.91148 54154.8810
00005 6.84 0.30 105.40 0.292 0.83 True 2 2 2.80221 2.61512 21.24749 53942.5128
00005 6.84 0.30 104.53 0.297 0.84 True 2 1 2.45474 2.25927 23.63201 54119.4646

Notes. The full version of the table is available in electronic form at the CDS. The albedos were computed from the absolute asteroid magnitudes H taken from Oszkiewicz et al. (2011). Entries with “True” in the “Fit” column indicate that the beaming parameter was fitted; otherwise, the value was computed from Eq. (1). On the other hand, the diameters were always fitted. Columns n9 and n18 refer to the number of observationsfitted in the 9-μm and 18-μ bands, and r, Δ, and α are the heliocentric and geocentric distances and phase angle, respectively. MJD is the modified Julian date of the last observation of the group. Typical minimum uncertainties are higher when the beaming parameter could not be fitted, as discussed in the main text.

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