高能脉冲可见光激光器在各种应用中都有很高的需求,包括但不限于光学显微镜 [ 1 ]、激光显示器 [ 2 – 4 ]、医疗应用 [ 5 ] 和激光通信 [ 6 ]。此外,高功率、高光束质量的红光激光器可以作为掺杂 Cr 3 和 Ho 3 离子的透明材料的泵浦源,例如 Cr:LiSAF(Cr 3 :LiSrAlF 6 )[ 7 ] 和 Ho:ZFG(Ho 3 掺杂的氟化锆玻璃)[ 8 ]。早期研究中,产生红光常用的技术是利用非线性光学晶体如KTP(KTiOPO 4 )、LBO(LiB 3 O 5 )等,通过Nd 3 掺杂激光晶体产生1.3 μm基频激光[9,10]。该方法已被许多研究者报道,利用Q开关操作调节脉冲宽度,输出功率大多在数百毫瓦范围内。到目前为止,已报道了一些稀土离子掺杂晶体,如Pr 3 、Dy 3 和Sm 3 离子,在红色光谱区产生有效发射[11]。近年来,通过蓝色激光源泵浦Pr 3 掺杂激光材料直接产生红光技术发展迅速,具有结构紧凑、转换效率高、稳定性好等优点。 Pr3掺杂材料由于其大的发射截面和四能级激光系统可见光跃迁,已被证明是直接产生可见激光辐射最有效的解决方案之一[12]。
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