掺Pr3+光纤激光器的泵浦脉冲诱导交叉相位调制锁模

D. Peter, G. Onishchukov, W. Hodel, H. Weber
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摘要

本文首次报道了一种同步泵浦锁模掺镨镝光纤激光器,激光器发射波长为~1.3µm。锁模是通过周期性相位调制实现的,该相位调制是由有源光纤中的泵浦脉冲诱导的交叉相位调制产生的。实验中使用的泵浦源是Nd:YAG激光器,以82 MHz的重复频率产生90 ps脉冲。光纤激光腔长度为泵浦激光腔长度的1倍(9倍)。活性光纤为长8 m的掺镨ZBLAN光纤,掺杂浓度为1000ppm,纤芯直径为4.8 pm,截止波长为~1µm。1064 nm处的吸收约为0.2 dB/m。光纤激光器通常在耦合泵浦功率约400mw时达到阈值。尽管光纤激光器被泵浦在吸收带的极长波翼,但耦合泵浦功率为~1 W的连续波输出功率为20 mW。由于掺镨光纤在1.3 pm处具有很强的(正常)群速度色散,当腔内不使用色散补偿元件时,产生的脉冲远不受带宽限制。然而,这些脉冲的光谱宽度为~1.2 nm,这表明使用色散补偿可以获得ps范围内的脉冲持续时间。详细介绍了光纤激光器的连续波和锁模特性。将交叉相位调制锁模方法与声光调制器损耗调制等锁模技术进行了比较。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Mode-locking of a Pr3+-doped fibre laser by pump pulse induced cross phase modulation
We report for the first time on a synchronously pumped mode-locked praseo-dymium-doped fluoride fibre laser emitting at~1.3µm. Mode-locking is achieved by a periodic phase modulation, which results from cross-phase modulation induced by the pump–pulses in the active fibre. The pump source used in the experiments is a Nd:YAG laser generating 90 ps pulses at a repetition rate of 82 MHz. The fibre laser cavity length is matched to a multiple of the pump laser cavity length (9 times). The active fibre is an 8-m-long praseodymum-doped ZBLAN fibre with a dopant concentration of 1000 ppm, a core diameter of 4.8 pm, and a cutoff wavelength of~1µm. The absorption at 1064 nm is approximately 0.2 dB/m. The fibre laser typically reaches threshold for ~400 mW of coupled pump power. Despite the fact that the fibre laser is pumped in the extreme long-wavelength wing of the absorption band, a cw output power of 20 mW is obtained for a coupled pump power of ~1 W. Because of the strong (normal) group velocity dispersion at 1.3 pm in the praseodymium-doped fibre, the generated pulses are far from bandwidth limited, when no dispersion compensating elements are used in the cavity. However, the spectral width of these pulses is ~1.2 nm, which shows that pulse durations in the ps range can be obtained using dispersion compensation. Details of the cw and the modelocking characteristics of the fibre laser are presented. The method of modelocking by cross-phase modulation is compared with other mode-locking techniques such as loss modulation using an acousto-optic modulator.
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