I. Introduction
Mode-Locked fiber lasers are a key source of subpicosecond optical pulses. Absorption spectrum of SWNTs prepared by the “high-pressure CO conversion method” in CNI. The absorption peak covers 1300-nm spectral range, and has a depth of 5%. Among typical mode-locking schemes, passive mode-locking (especially using a saturable absorber) is attractive due to its structural simplicity and fast recovery time, resulting in fast loss modulation inside of the cavity and much shorter pulses compared with active mode-locking [1].