Fig. 10.

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Magnitudes of the azimuthal velocity components vϕ of 4 M⊙ HVSs in Newtonian gravity as a function of their radial coordinates, r, at the time of observation for a prolate dark matter halo with axis of symmetry in the plane of the disk. The light blue and purple dots show the HVSs for a halo with (qy, qz) = (1.1, 1) and (qy, qz) = (1.2, 1), respectively. The black line shows the upper limit of |vϕ| in QUMOND due to the triaxial bulge. The upper limit also holds for HVSs with masses lower than 4 M⊙, provided they are beyond a certain galactocentric distance, e.g., r ≳ 30 kpc (50 kpc) for 3 M⊙ (2.5 M⊙) HVSs.
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