“…Compared with Q-switching, mode-locking attracted more considerable attention because of narrower pulse width and higher peak power. Recently, various kinds of two-dimensional (2D) materials, such as graphene [ 8 , 9 ], graphene oxide (GO) [ 10 ], MXenes [ 11 ], single-walled carbon nanotubes (SWCNTs) [ 12 ], quantum wells (QWs) [ 13 ], black phosphorus (BP) [ 14 ], topological insulators (TIs) [ 15 , 16 , 17 ], transition metal dichalcogenides (TMDCs) [ 18 , 19 , 20 , 21 , 22 , 23 , 24 ], and layered metal sulfides (LMSs) [ 25 ] were widely used as saturable absorbers in mode-locked fiber lasers due to their outstanding nonlinear saturable absorption properties caused by sub-band gap absorption or the Pauli blocking principle [ 26 ]. In particular, various TMDCs including MoS 2 [ 19 ] and WS 2 [ 21 ], etc.…”