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Table 2

Best-fit parameters for the Genoid model (Sect. 4.1) and the three dynamical models described in Sect. 4.2: Keplerian; multipole; multipole with fixed spin-axis pole.

Var. Unit Genoid val. σ Keplerian val. Multipole val. Fixed-pole val. σ
m1 1018 kg 7.72 0.61 7.75 7.78 7.80 0.26
m2 1016 kg 0 0 4.72 4.71 3.96
P day 3.595678 0.00002 3.595758 3.604302 3.604280 0.008544
e 0.002 0.005 0.005 0.005 0.010
i deg 93.9 2.6 87.356 88.104 86.232 1.0
a km 1080 28
Ω deg 285.5 1.8
ω deg 154 20
tp JD 2452215.18338 0.20374
Ω1 deg 15.8 15.9 15.5 1.0
ϖ1 deg 327 326 327 10
λ1 deg 206.3 206.3 206.0 1.0
λpole deg 195.8 1.5 195.6 195.1 1.0
βpole deg 2.3 2.8 2.2 3.3 1.0

RMS mas 8.1
202 226 278
453 460 448

Notes. For the Genoid method, the orbital elements of Linus are expressed in EQJ2000. For the multipole method they are osculating for the epoch T0 = 2454047.326750 JD and expressed in the standard stellar reference frame. If the orbit lies in the equatorial plane of body 1, they fulfill i = 90° − bpole, Ω = 180° + lpole · m1 denotes the mass of body 1 (i.e., Kalliope), m2 body 2 (moon), P the orbital period of the orbit, e eccentricity, i inclination, a semi-major axis, Ω longitude of the ascending node, ω argument of pericenter, tp time of pericenter, Ω1 longitude of node, ϖ1 longitude of pericenter, λ1 true longitude, λpole ecliptic longitude of Kalliope’s rotation pole, βpole ecliptic latitude, RMS of residuals for the 113 measurements given in Table B.3, and are defined in Appendix A.

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