Babin S A, Vatnik I D, Laptev A Yu, Bubnov M M, Dianov E M
Opt Express. 2014 Oct 20;22(21):24929-34. doi: 10.1364/OE.22.024929.
Cascaded lasing provided by Raman gain (at 1115-nm pumping) and random distributed feedback (via Rayleigh backscattering) in a 1.65-km phosphosilicate fiber is studied. Output power for the second Stokes component (1398 nm) exceeds 5 W at pump power of 11 W. In contrast to conventional cascaded Raman laser with high-Q cavity for the intermediate first Stokes component, there is no cavity here and no cavity losses, correspondingly. Longitudinal power distribution is shown to be quite different also. As a result, the efficiency of pump to 2nd Stokes wave conversion is not influenced by the intermediate stage and depends only on the integral attenuation in the fiber. Herewith, the number of generated 2nd Stokes photons at the output may even exceed the absorbed pump photons due to the lower attenuation of Stokes waves.
研究了在1.65公里长的磷硅光纤中由拉曼增益(在1115纳米泵浦下)和随机分布反馈(通过瑞利背散射)提供的级联激光。在11瓦的泵浦功率下,第二斯托克斯分量(1398纳米)的输出功率超过5瓦。与用于中间第一斯托克斯分量的具有高Q腔的传统级联拉曼激光器不同,这里没有腔,相应地也没有腔损耗。纵向功率分布也显示出相当不同。结果,泵浦到第二斯托克斯波转换的效率不受中间阶段的影响,仅取决于光纤中的积分衰减。因此,由于斯托克斯波的较低衰减,输出处产生的第二斯托克斯光子数甚至可能超过吸收的泵浦光子数。