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Spatial coherence of the Stokes component of stimulated Raman scattering excited in a long multimode fibre

机译:长多模光纤中受激拉曼散射的斯托克斯分量的空间相干性

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The mode structure of the Stokes component of stimulated Raman scattering (SRS) in a multimode fibre excited by a pump field with statistics corresponding to a narrowband Gaussian noise model is theoretically analysed. The relation is obtained between the number of spatially coherent radiation modes of the Stokes wave and fibre parameters and SRS excitation conditions. It follows from this relation that the degree of spatial coherence of the Stokes radiation at the fibre output is determined by the number of spatial modes of pump radiation and the averaged gain of the Stokes radiation over the interaction length. It is established that there exists the threshold gain at which the number of spatially coherent radiation modes of the Stokes component increases infinitely and, therefore, its spatial coherence tends to zero. The estimates of the number of spatially coherent radiation modes of the Stokes component showed that already at the Raman scattering excitation threshold their number is so great that the degree of spatial coherence of the Stokes component radiation corresponds to the degree of coherence of a thermal source radiation. The measured dispersion of spatial intensity fluctuations of the Stokes component separated by using an interference filter (with the transmission bandwidth similar to 1 nm at 620 nm) proved to be approximately three times higher than the dispersion of radiation intensity fluctuations of a luminescent lamp. The large dispersion of spatial intensity fluctuations of the Stokes component is caused most likely by individual intensity spikes in a small-scale (unresolved by a detector with a spatial resolution of similar to 14 mu m) speckle pattern produced in the detection plane by monochromatic Stokes radiation.
机译:理论上分析了由泵浦场激发的多模光纤中受激拉曼散射(SRS)的斯托克斯分量的模结构,该统计具有与窄带高斯噪声模型相对应的统计量。在斯托克斯波的空间相干辐射模式的数量与光纤参数和SRS激发条件之间获得关系。从该关系得出,光纤输出处斯托克斯辐射的空间相干程度由泵浦辐射的空间模式数量和相互作用长度上斯托克斯辐射的平均增益确定。确定存在阈值增益,在该阈值增益处,斯托克斯分量的空间相干辐射模的数量无限增加,因此,其空间相干性趋于零。对斯托克斯分量的空间相干辐射模式数量的估计表明,在拉曼散射激发阈值处,它们的数量是如此之大,以至于斯托克斯分量辐射的空间相干程度与热源辐射的相干程度相对应。 。事实证明,通过使用干涉滤光片(传输带宽在620 nm处类似于1 nm)分离出的斯托克斯分量的空间强度波动的色散大约是荧光灯辐射强度波动的色散三倍。 Stokes组件的空间强度波动的较大分散很可能是由单色Stokes在检测平面上产生的小尺寸斑点斑点(由空间分辨率近似于14μm的检测器无法分辨)引起的,这些斑点斑点在检测平面中产生辐射。

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