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Fig. B.1

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Frequency spectra and determined fundamental (fund.) orbital frequencies of the orbit of a randomly chosen HS’ star in the fiducial potential (see Appendix A) for an integration time of 100 Gyr, outputted each 10 Myr. The filtered (filt.) spectra for ΩRϕ) correspond to spectra out of which the multiples of Ωz and Ωϕz) are filtered. For ΩR, we see that the leading frequency of the spectrum is twice Ωz. However, the orbit’s phase-space distribution does not suggest it is a resonant orbit, and this value for ΩR does not fall within the range absR : Ωz − 0.7) < 0.15), and it is valid to choose the next-highest peak as fundamental ΩR.

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