Self-switching fiber loops imbalance by fiber dispersion

W. Wong, Mordehai Margalit, S. Namiki, S. Longhi, E. Ippen, H. Haus
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Abstract

Using stimulated Brillouin scattering (SBS) in glass fibers as phase-conjugating process, the field of application of SBS phase conjugators' can be expanded, because fibers offer a lowpower threshold and a stable performance even at high input energies in contrast to liquid and gas SBS phase conjugators. Undoped multimode quartz fibers with a core diameter of 200 pm were tested as phase conjugators with high fidelity and reflectivity for 1064-nm wavelength in Ref. 2. Only the first two meters of a fiber contribute constructively to the stimulated Brillouin scattering process for input pulses with a coherence length of about 50 cm, so that attenuation in the fiber plays only a secondary role. Therefore, fibers with higher attenuation at shorter wavelengths can be still used as phase conjugators. We present results of fiber phase conjugators at three wavelengths from near-infrared 1.06 pm over visible 532 nm to nearultraviolet 355 nm. The SBS threshold, reflectivity and fidelity were characterized. Commercial all-silica multimode quartz glass fibers with a step-index structure, a core diameter of 100 pm and a cladding diameter of 110 pm were used. The core is made from undoped quartz glass. The numerical aperture NA is 0.22, which corresponds to a maximum full angle of 25.4' (-440 mrad) for coupling light into the fiber. The lengths of all investigated fibers were more than 2 m. The attenuation of the used fibers is about 2 dB/km at 1064 nm, 30 dB/km at 532 nm and 45 dB/km at 355 nm. At a fiber length of 2 meters, losses of about 0.2% at 1064 nm, 3% at 532 nm and 4% at 355 nm are expected for a pulse traveling forth and back the fiber. Figure 1 shows the experimental setup for our investigations. A NdYAG oscillator-
由光纤色散引起的自交换光纤环路不平衡
利用玻璃纤维中的受激布里渊散射(SBS)作为相位共轭过程,可以扩大SBS相位共轭器的应用领域,因为与液体和气体SBS相位共轭器相比,光纤具有低功率阈值,即使在高输入能量下也具有稳定的性能。在文献2中,对芯径为200pm的未掺杂多模石英光纤作为相位共轭器进行了高保真度和1064nm波长反射率的测试。对于相干长度约为50 cm的输入脉冲,只有光纤的前两米对受激布里渊散射过程有建设性的贡献,因此光纤中的衰减仅起次要作用。因此,在短波长处具有较高衰减的光纤仍然可以用作相位共轭器。我们给出了光纤相位共轭器在近红外1.06 pm /可见光532 nm至近紫外355 nm三个波长的结果。对SBS阈值、反射率和保真度进行了表征。采用阶梯折射率结构的全硅多模石英玻璃纤维,芯径为100 pm,包层直径为110 pm。核心由未掺杂的石英玻璃制成。数值孔径NA为0.22,对应于耦合光进入光纤的最大满角为25.4' (-440 mrad)。所测纤维长度均大于2 m。所使用的光纤在1064 nm处衰减约为2 dB/km,在532 nm处衰减约为30 dB/km,在355 nm处衰减约为45 dB/km。在长度为2米的光纤中,脉冲在1064 nm处的损耗约为0.2%,在532 nm处的损耗为3%,在3555 nm处的损耗为4%。图1显示了我们研究的实验设置。一个NdYAG振荡器
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