Limits of Performance of a Nd3+-Doped Fiber Amplifier at 1.3 μm

M. Dakss, W. Miniscalco
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Abstract

There has been a continuing interest in developing fiber amplifiers for the 1.3 μm window which is used for most optical communications traffic. Neodymium-doped fibers remain potential candidates for this function despite the problem of excited state absorption (ESA) near 1.3 μm which can lead to loss rather than gain, particularly at shorter wavelengths [1]. The effects of ESA are known to be a function of glass composition: Aluminum/phosphorus-doped silica [2-4] and phosphate glass [5] exhibit gain at shorter wavelengths than Ge-doped silica, and fluorozirconate glass has provided gain at wavelengths as short as 1.32 μm [6-9]. Despite these results, the practicality of Nd3+-doped fiber amplifiers is still in question. We have addressed this issue by constructing a fiber amplifier model which exploits the availability of measured cross sections for a wide variety of Nd3+-doped glasses.
1.3 μm掺Nd3+光纤放大器的性能极限
人们一直对开发用于大多数光通信业务的1.3 μm窗口的光纤放大器感兴趣。尽管在1.3 μm附近存在激发态吸收(ESA)问题,但掺钕光纤仍然是该功能的潜在候选者,这可能导致损耗而不是增益,特别是在较短波长[1]。众所周知,ESA的影响是玻璃成分的函数:铝/磷掺杂的二氧化硅[2-4]和磷酸盐玻璃[5]在较短的波长下比锗掺杂的二氧化硅表现出增益,氟锆酸盐玻璃在短至1.32 μm的波长下提供增益[6-9]。尽管有这些结果,掺Nd3+光纤放大器的实用性仍然存在问题。我们通过构建一个光纤放大器模型来解决这个问题,该模型利用了各种Nd3+掺杂玻璃的测量截面的可用性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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