《Table 1.Saturable Absorption Properties for Different Nanomaterial-Based SAs at 1.5μm and Mode-Lock

《Table 1.Saturable Absorption Properties for Different Nanomaterial-Based SAs at 1.5μm and Mode-Lock   提示:宽带有限、当前游客访问压缩模式
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《Q-switched and mode-locked Er-doped fiber laser using PtSe_2 as a saturable absorber》


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Due to the polarization-dependent characteristics of SA,the above-mentioned laser can be switched from a Q-switched state to a mode-locked state by adjusting the polarization state.Mode-locked pulses are generated when the pump power increases to about 80 m W.The stable mode-locked state maintains at even pump power up to a maximum of 450 mW,and the output single pulse energy can be up to 0.53 nJ.Figure 6shows typical output characteristics of the mode-locked laser with a pump power of 250 mW.As presented in Fig.6(a),the pulse repetition rate is about 23.3 MHz,which matches the cavity length well and indicates that the laser is working in the mode-locked state.Figure 6(b)is the pulse autocorrelation trace that can be well fitted by the hyperbolic secant function with a width of 1.58 ps,which indicates the real pulse width of approximately 1.02 ps.Figure 6(c)is the corresponding optical spectrum,whose 3 dB bandwidth is~6 nm,and the center wavelength is 1563 nm.There are four groups of sidebands on both sides of the center wavelength,which shows a clear characteristic of the traditional negative dispersion soliton and is consistent with our calculation of the net dispersion in the resonant cavity.The radio-frequency(RF)spectrum of the mode-locking state is measured and shown in Fig.6(d)with a resolution bandwidth of 300 kHz.The signal-to-noise ratio(SNR),which is up to 61 d B,shows that the fiber laser operates in a highly stable regime.To confirm the long-term stability of the mode-locked operation,fluctuation of the 3 d B spectral bandwidth is measured and shown in the inset of Fig.6(c).The results show that the mode-locked pulses can be stable for hours.The durations of the mode-locked laser pulses are comparable to those of the reported lasers mode-locked with other nanomaterials as shown in Table 1,which indicates that PtSe2is a strong competitor for acting as an SA.To confirm the contribution of the PtSe2-based SA to mode-locking operation,we remove the PtSe2film covering the microfiber and just cover the microfiber with a piece of PDSM,which is the same as the one supporting the PtSe2film.By carefully adjusting the PC and pump power,no laser pulses can be observed in this case.Therefore,the mode-locking operation is caused by the PtSe2-based SA.Owing to the PtSe2-covered-microfiber structure,PtSe2interacts with the evanescent field of light waves outside the microfibers.Therefore,this PtSe2-based SA has relatively high damage threshold.Also,the PtSe2was not damaged during our experiment.