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

被引:60
作者
Jackson, SD [1 ]
King, TA [1 ]
机构
[1] Univ Manchester, Schuster Lab, Dept Phys & Astron, Laser Photon Grp, Manchester M13 9PL, Lancs, England
基金
英国工程与自然科学研究理事会;
关键词
laser excitation; lasers; modeling; neodymium : YAG lasers; optical fibers; pulsed lasers;
D O I
10.1109/3.668764
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
We present the results from experiments relating to a gain-switched Tm-doped silica fiber laser in which a gain-switched Nd:YAG laser is used to pump the H-3(5) energy level of the Tm3+ dopant ion. This fiber laser configuration is the first example to our knowledge of a moderate energy gain-switched fiber laser which is pumped with a low-repetition-rate high-energy pulsed laser. For a near-optimized cavity, the gain-switched fiber laser produces a maximum pulse energy of 1.46 mJ at a maximum linear slope efficiency of 20% and a total optical-to-optical efficiency (with respect to the launched energy) of 19%. At low pump energies, the slope efficiency is approximately 40%, however, saturation of the output pulse energy is observed with the increase in the launched pump energy. We also present results from a numerical model that simulates H-3(5)-band pumping and includes all of the known pump excited-state absorption (ESA) mechanisms and, in addition, four cross-relaxation mechanisms have also been included. The calculations establish that the pump ESA mechanism contributes only a small loss factor to the overall efficiency of the laser when the Tm-doped silica fiber laser is pumped at low pump energies, however, as the pump energy is increased, losses due to pump ESA limit the amount of output energy from the fiber laser, The loss mechanism is mainly attributed to pump ESA from the H-3(4) upper laser level to the combined F-3(2.3) energy level at low launched pump energies because of the large absorption cross section for this transition and the relatively long Lifetime of the H-3(4) energy level. For harder pumping conditions, the majority of the excited state population resides in the (1)G(4) level, inhibiting in some laser configurations gain-switching of the fiber laser until cessation of the pump pulse itself.
引用
收藏
页码:779 / 789
页数:11
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