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Femtosecond inscribed mode modulators in large mode area fibers -experimental and theoretical analysis

机译:大型地区纤维的飞秒铭刻模型 - 经验性和理论分析

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We present the experimental and theoretical analysis of a mode modulator in a few mode LMA fiber. The mode modulator consists of a section with a modified refractive index alongside the fiber core in the cladding, disturbing the guidance of the modes in the core. The extent of excitation of these disturbed modes depends on the overlap of the excited undisturbed and disturbed modes. At the end of the modulator, undisturbed modes will be excited again in the fiber core, in dependency of the spatial field distribution of the disturbed modes at the boundary. In the mode modulator disturbed higher order modes lead to modal interference, causing a dependency of the spatial distribution of the light in the mode modulator on the propagation length of the disturbed modes. Hence, the modal output field depends on the length of the mode modulator. For the experiments, the mode modulator was inscribed directly into the LMA fiber with ultrashort laser pulses. During the inscription process the modal content at the end of the fiber was measured using a computer generated hologram as a correlation filter. In dependency of the length of the modulator strong oscillations between the content of the fundamental and the higher order modes are observable. In the case of an initially excited fundamental mode, its content could be reduced to below 5%, whereat the content of the LP11 modes was up to 90%. While measurement and simulation show qualitative agreement, differences are caused by inhomogeneities of the refractive index modifications.
机译:我们在几种模式LMA光纤中介绍了模式调制器的实验和理论分析。模式调制器由具有改进的折射率的部分组成,该截面沿着纤维芯在包层中,扰乱了核心中模式的引导。这些扰动模式的激发程度取决于激发不受干扰和干扰模式的重叠。在调制器的末端,在光纤核心中再次激发未受干扰的模式,其依赖于边界处的受扰动模式的空间场分布。在模式调制器中,受扰动的更高阶模式导致模态干扰,导致光线分布在扰动模式的传播长度上的模式调制器中的空间分布。因此,模态输出字段取决于模式调制器的长度。对于实验,模式调制器直接刻入LMA纤维中,用超短的激光脉冲。在铭文过程期间,使用计算机生成的全息图作为相关滤波器测量光纤末端的模态内容。依赖于调制器的长度强大的振荡之间的基本和高阶模式的含量是可观察到的。在最初激励的基本模式的情况下,其含量可以降低至低于5%,但LP11模式的含量高达90%。虽然测量和模拟显示定性协议,但差异是由折射率修饰的不均匀性引起的。

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