I. Introduction
Ultrashort laser pulses at multi-GHz repetition rates have been widely applied for scientific researches and industrial applications, including high-speed nonlinear imaging [1], dual-comb spectroscopy [2], [3], coherent optical communication [4], [5], low-noise microwave generation [6], high throughput micromachining [7], [8], [9], [10], etc. High-repetition-rate (HRR) mode-locked fiber laser, as one of the promising technologies for generating multi-GHz ultrashort pulses, has been paid special attention [11], [12], [13], [14], [15], and fundamental repetition rates of up to >10 GHz have been reported at different wavelengths [16], [17], [18]. The ultrashort cavity design of HRR mode-locked fiber lasers, on the other hand, inherently imposes restrictions on manipulating the performance of mode-locking, particularly the tunability of central wavelength and transform-limited pulsewidth, which prevents their applications in the fields requiring wavelength sweeping and pulsewidth tuning [19], [20], [21], [22], [23].