Data for time-averaged dipolarity from all runs of this paper as a function of compensated shear Rossby number (i.e., Ro_sh/Ro_conv^ℓ) and normalized by its critical value given in Eq. (7). All transitions from dipolar to oscillatory branches collapse on each other. The branch that does not follow the trend is the special case of g ∝ r and the high Ra values (run gr_2 in Table B.1, see Fig. 5d and discussion in Sect. 4.3). Colors, symbols, and lines are the same as in Fig. 7.