“…Since the soliton state exists on the lower branch of the Kerr-bistability curve, it is generally only accessible with decreasing pump frequency [39,40]. Except for the recent discoveries of special conditions (e.g., soliton crystals [41,42], breathing solitons [43], dark pulses in a normal dispersion [44][45][46]), microcombs can be mainly divided into three different states, a primary comb (i.e., Turing pattern or Turing roll), chaotic modulation instability (MI), and a dissipative Kerr soliton (DKS) [47]. The essential difference between the former two states and a soliton state is effective pump detuning, and effective red detuning results in a low soliton conversion efficiency compared with that obtained with the MI comb [19].…”