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Efficient gain-switched operation of a Tm-doped silica fiber laser

机译:掺Tm的石英光纤激光器的高效增益切换操作

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We present the results from experiments relating to angain-switched Tm-doped silica fiber laser in which a gain-switchednNd:YAG laser is used to pump the 3H5 energy levelnof the Tm3+ dopant ion. This fiber laser configuration is thenfirst example to our knowledge of a moderate energy gain-switched fibernlaser which is pumped with a low-repetition-rate high-energy pulsednlaser. For a near-optimized cavity, the gain-switched fiber lasernproduces a maximum pulse energy of 1.46 mJ at a maximum linear slopenefficiency of 20% and a total optical-to-optical efficiency (withnrespect to the launched energy) of 19%. At low pump energies, the slopenefficiency is approximately 40%, however, saturation of the output pulsenenergy is observed with the increase in the launched pump energy. Wenalso present results from a numerical model that simulates 3Hn5-band pumping and includes all of the known pumpnexcited-state absorption (ESA) mechanisms and, in addition, fourncross-relaxation mechanisms have also been included. The calculationsnestablish that the pump ESA mechanism contributes only a small lossnfactor to the overall efficiency of the laser when the Tm-doped silicanfiber laser is pumped at low pump energies, however, as the pump energynis increased, losses due to pump ESA limit the amount of output energynfrom the fiber laser. The loss mechanism is mainly attributed to pumpnESA from the 3H4 upper laser level to the combinedn3F2,3 energy level at low launched pump energiesnbecause of the large absorption cross section for this transition andnthe relatively long lifetime of the 3H4 energynlevel. For harder pumping conditions, the majority of the excited statenpopulation resides in the 1G4 level, inhibiting innsome laser configurations gain-switching of the fiber laser untilncessation of the pump pulse itself
机译:我们介绍了与增益转换Tm掺杂石英光纤激光器相关的实验结果,其中增益转换nNd:YAG激光器用于泵浦Tm3 +掺杂离子的3H5能级n。因此,这种光纤激光器配置是我们了解的一个中等能量增益转换光纤激光器的第一个示例,该激光器被低重复频率高能量脉冲激光泵浦。对于接近最佳的腔,增益转换光纤激光器在最大线性斜率效率为20%时产生的最大脉冲能量为1.46 mJ,总光光效率(不考虑发射能量)为19%。在低泵浦能量下,斜率效率大约为40%,但是,随着所发射泵浦能量的增加,观察到输出脉冲能量的饱和。 Wen还提出了一个数值模型的结果,该数值模型模拟了3Hn5波段的泵激,并包括所有已知的泵激态吸收(ESA)机制,此外,还包括了四跨弛豫机制。计算结果表明,当在低泵浦能量下泵浦掺Tm的硅纤维激光器时,泵浦ESA机理仅对激光器的整体效率造成很小的损失,但是,随着泵浦能量的增加,由于泵浦ESA造成的损耗限制了从光纤激光器输出能量。损耗机理主要归因于在低发射泵浦能量下从3H4上激光能级泵浦到3n2F2,3能级的泵浦能级,这是因为过渡过程的吸收截面大,并且3H4能级的寿命相对较长。对于更困难的泵浦条件,大多数激发态种群处于1G4能级,从而抑制了光纤激光器的一些激光器配置的增益切换,直到需要泵浦脉冲本身为止

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