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Table 1

List of new asteroid models derived from combined dense and sparse data or from sparse data alone.

Asteroid λ 1 β 1 λ 2 β 2 P N lc N app N 689 N 703 N 950
[deg] [deg] [deg] [deg] [hours]

243 Ida 259 −66 74 −61 4.633632 53 6 134 122 25
364 Isara 282 44 86 42 9.15751 4 1 98 104
540 Rosamunde 301 81 127 62 9.34779 3 1 135 83
550 Senta 63 −40 258 −58 20.5726 9 1 151 85
553 Kundry 197 73 359 64 12.6025 5 1 61 80
621 Werdandi 247 −86 66 −77 11.77456 12 2 146 71
936 Kunigunde 47 57 234 50 8.82653 154 88
951 Gaspra 20 23 198 15 7.042027 71 4 117 89
1286 Banachiewicza 214 62 64 60 8.63043 81 51
1353 Maartje 266 73 92 57 22.9926 154 139
1378 Leonce 210 −67 46 −77 4.32527 89 113
1423 Jose 78 −82 12.3127 121 134
1446 Sillanpaa 129 76 288 63 9.65855 2 1 76 73
1464 Armisticia 194 −54 35 −69 7.46699 2 1 231 67
1503 Kuopio 170 −86 27 −61 9.9586 116 68
1527 Malmquista 274 80 14.0591 49 107
1618 Dawn 39 −60 215 −51 43.219 93 91
1633 Chimay 322 77 116 81 6.59064 2 1 127 83
1691 Oort 45 68 223 58 10.2684 86 60
1703 Barry 46 −76 221 −71 107.04 89 138
1805 Dirikis 364 48 188 61 23.4543 117 91
1835 Gajdariya 34 74 204 69 6.33768 66 86
1987 Kaplan 357 −58 9.45950 8 2 81 28
2430 Bruce Helin 177 −68 129.75 15 1 112
3279 Solon 268 −70 8.1043 3 1 137
3492 Petra-Pepi 9 −57 202 −16 46.570 15 1 25 111
4399 Ashizuri 266 −48 45 −61 2.830302 4 1 20 84
4606 Saheki 44 59 222 68 4.97347 6 1 123
6159 1991 YH 266 67 62 67 10.6590 3 1 102
6262 Javid 93 76 275 69 8.02054 3 1 106
6403 Steverin 246 77 109 73 3.49119 2 1 74
7043 Godart 73 62 235 80 8.4518 4 1 121
7169 Linda 11 −60 198 −61 27.864 5 1 95

Notes. For each asteroid, the table gives the ecliptic coordinates λ1 and β1 of the pole solution with the lowest χ2, the corresponding mirror solution λ2 and β2, the sidereal rotational period P, the number of dense lightcurves Nlc observed during Napp apparitions, and the number of sparse data points for the corresponding observatory: N689, N703, and N950. The uncertainty of the sidereal rotational period corresponds to the last decimal place of P and of the pole direction to 5–10° if we have multi-apparition dense data or 10–20° if the model is based mainly on sparse data (i.e., only a few dense lightcurves from 1–2 apparitions).

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