红外光纤材料

J.A. Savage
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引用次数: 39

摘要

本文从20世纪60年代早期的氧化玻璃、硫系玻璃和晶体卤化物的研究进展出发,论述了纤维材料的发展。通过硅酸盐纤维的巨大发展,这导致了我们今天新的红外光通信能力;介绍了中红外氟化玻璃纤维和远红外玻璃、空心芯和结晶纤维的最新研究进展。光纤制造技术在20世纪70年代迅速发展,使近红外波长的损耗达到了每公里1分贝的一小部分。在20世纪80年代,使用工作在0.8-0.9 μm、1.3 μm和1.55 μm的近红外多模硅酸盐玻璃纤维以及工作在1.3 μm和1.55 μm的单模光纤,光通信成为可能。这些光纤在1.55 μm处的损耗约为0.2 dB/km,非常接近GeO2-SiO2玻璃的本质损耗极限。为了在比硅酸盐纤维更远的距离上实现无重复透射,有必要用低损耗介质制造纤维。在红外光谱区,材料的衰减主要是瑞利散射和多声子吸收。因此,如果材料可以传输到更远的红外可以利用,那么潜在的低得多的损失可以实现,因为瑞利散射具有λ−4依赖性。在2.55 μm波长的光纤中,有可能实现10−2 dB/km的损耗,而在3 ~ 4.5 μm波长的较长波长的光纤中,损耗可能更低。由于这些原因,研究人员现在正在解决从氟锆酸盐和氟铪酸盐玻璃中制造中红外纤维的问题。远红外光谱区的光纤有非常不同的应用,主要要求传感器和电力输送设备的路径长度为几厘米到几米。尽管事实上只需要短长度的纤维,但要找到足够低损耗的材料,同时又表现出机械和环境的完整性,还存在一些问题。硫系玻璃、空心氧化玻璃、单晶卤化物和多晶卤化物正在进行研究,因为没有明显的前端运行材料能够满足所有要求。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Materials for infrared fibre optics

This review discusses the development of materials for fibres from early work in the 1960s on oxide glass, chalcogenide glass and crystalline halides which was way ahead of its time; through the huge development on silicate fibres which has led to our present-day new IR optical communications capability; to the frontiers of current research on mid IR fluoride glass fibres and far IR glass, hollow core and crystalline fibres. Fibre fabrication technology was rapidly developed during the 1970s allowing losses of a fraction of a dB/km to be achieved at near infrared wavelengths. In the 1980s optical communications have become possible using multimode silicate glass fibres in the near IR operating at 0.8-0.9 μm, at 1.3 μm and at 1.55 μm and using monomode fibres operating at 1.3 μm and 1.55 μm. The loss in these fibres at 1.55 μm is about 0.2 dB/km which is very nearly the intrinsic loss limit of GeO2-SiO2 glass. To achieve repeaterless transmittance over longer distances than possible with silicate fibres it is necessary to fabricate fibre from a lower loss medium. In the infrared spectral region attenuation in a material is dominated by Rayleigh scattering and multiphonon absorption. Thus if materials transmitting farther into the infrared can be utilised then potentially much lower losses can be achieved since Rayleigh scatter has a λ−4 dependence. It may be possible to achieve of the order of 10−2 dB/km loss in a fibre at 2.55 μm and perhaps lower losses at longer wavelengths of 3 to 4.5 μm. For these reasons researchers are now addressing the problems of making mid IR fibres from amongst the fluorozirconate and fluorohafnate glasses. There are very different applications for fibres in the far infrared spectral region mainly requiring path lengths of a few centimeters to a few meters for sensor and power delivery devices. In spite of the fact that only short lengths of fibre are required, there are problems in finding sufficiently low loss materials which also demonstrate mechanical and environmental integrity. Research is being carried out amongst the chalcogenide glasses, hollow core oxide glasses, monocrystalline halides and polycrystalline halides since there is no obvious front running material which is able to satisfy all requirements.

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