Fig. 10

Example of the one-dimensional χ2 mapping used to derive uncertainties of orbital elements for the ξ Tau system. The dependencies of the χ2 values on the three nodes Ω1, Ω2, Ω3 are shown, while the remaining elements correspond to the best-fit values from Table 15. The preferred solution for Ω1 ≃ 331°, with χ2 = 2578, and a hint of a mirror solution at Ω1 ≃ 151° are clearly visible. If the latter is optimised separately, we would obtain χ2 as low as 2 749. The sudden increase of corresponds to the disappearance of the eclipses of the inner binary, which naturally results in extreme O−C’s.
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