“…An essential feature is that only the harmonic orders of n = 6m ± 1 (m = 1, 2, 3, · · · ) are present, while other harmonic orders are all suppressed. This interesting feature looks similar to the cases of HHG driven by two-color counter-rotating circularly polarized laser fields from gases [4,52,53] or plasmas [54], where spectral selection rules of n = 3m ± 1 can be deduced from simple arguments based on three-fold symmetry and conservation laws for energy, parity, and spin angular momentum [4,19,[52][53][54]. The situation is different here, since a single circularly polarized driver is used.…”