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Gain competition in Yb-doped symmetry-free photonic crystal fibers under severe heat load

机译:严重热负荷下掺Yb的无对称光子晶体光纤的竞争

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Summary form only given. In the last few years Yb-doped Photonic Crystal Fibers (PCFs) have become the key component for the development of reliable and high-performance lasers [1]. Despite an effective cooling of the fiber medium, a significant heat density is generated when high pump power is involved, which alters the propagation of the modes, causing unwanted coupling and destroying the output beam quality [2]. Symmetry-Free PCFs (SF-PCFs), characterized by the absence of any mirror symmetry in the inner cladding, have shown interesting properties in terms of resilience to thermal effects [3]. In fact SF-PCFs provide a strong delocalization of the Higher-Order Mode (HOM) even under severe heat load, thus preventing its thermally-driven reconfinement in the core. As an unwanted side effect, a poor confinement of the Fundamental Mode (FM), due to its coupling with cladding modes, is obtained in the absence of thermal effects, which can negatively affect the fiber single-mode regime and potentially compromise the effectiveness of the amplification process.In this work the amplification properties of air-silica Yb-doped SF-PCFs have been analyzed with a simulation tool which comprises a FEM-based full-vector modal solver, to calculate the propagating mode fields, an amplifier model, which accounts for the power evolution, and a thermal model, to obtain the temperature distribution and the consequent refractive index change in the fiber cross-section [4]. The 19-cell core SF-PCF considered in this analysis, whose cross-section is shown in the inset of Fig. 1(a), is built over a triangular lattice with pitch Λ = 15 μm and normalized air-hole diameter d/Λ = 0.5. The interaction between FM and first HOM at 1032 nm, induced by both thermal effects and amplification process, has been studied for fibers with inner cladding diameter dIC between 15Λ and 19Λ, while the air-cladding thickness is fixed at 7 μm. A co-propagating pumping scheme, with 400 W of pump power at 976 nm, has been considered for the 1-m long fiber amplifier with a pump absorption of 27 dB/m. The input power for the FM and the first HOM, defined as the LP
机译:仅提供摘要表格。在过去的几年中,掺Yb的光子晶体光纤(PCF)已成为开发可靠和高性能激光器的关键组件[1]。尽管有效地冷却了纤维介质,但在涉及高泵浦功率时仍会产生显着的热密度,这会改变模式的传播,造成不必要的耦合并破坏输出光束的质量[2]。无对称PCFs(SF-PCFs)的特征是在内包层中没有任何镜面对称性,因此在抵抗热效应方面表现出令人感兴趣的特性[3]。实际上,即使在严重的热负荷下,SF-PCF仍可提供高阶模式(HOM)的强大离域功能,从而防止了其在内核中的热驱动约束。由于不希望有的副作用,在没有热效应的情况下,由于其与包层模式的耦合,导致对基本模式(FM)的限制较弱,这可能会对光纤单模状态产生负面影响,并有可能损害光纤的单模性能。在这项工作中,已使用包括基于FEM的全矢量模态求解器的仿真工具分析了空气硅Yb掺杂的SF-PCF的放大特性,以计算传播模式场,放大器模型,其中考虑了功率演化和热模型,以获得纤维横截面中的温度分布和随之而来的折射率变化[4]。在此分析中考虑的19电池芯SF-PCF的横截面如图1(a)所示,是在间距Λ= 15μm,归一化气孔直径d /的三角形晶格上构建的Λ= 0.5。对于内包层直径dIC在15Λ和19 19之间,而空包层厚度固定为7μm的光纤,已经研究了由热效应和放大过程引起的FM和1032 nm处的第一HOM之间的相互作用。对于长度为1 m的光纤放大器,泵浦吸收为27 dB / m,已经考虑了在976 nm处具有400 W泵浦功率的共传播泵浦方案。 FM和第一个HOM的输入功率,定义为LP

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