“…DLSs were first used for particle acceleration in the late 1940s [42,43]. Since then, steady progress has been made including an increased frequency range from GHz to THz [12-15, 19, 44], comparable shunt impedance as the metallic disk-loaded structure by using low loss microwave ceramic materials [14,21], tunability with a second layer of nonlinear ferroelectric [15], higher order modes (HOMs) damping with segmented conducting boundaries [45], multipacting suppression by external magnetic field [46,47], and GV/m level gradient in rf breakdown tests [48] as well as CWA experiments [19], etc. Despite this progress, high power rf pulse generation beyond 100 MW with drive bunch train excitation in the TBA approach was yet to be demonstrated for DLS.…”