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COST 217 interlaboratory comparison of optical measurements on single-mode fibre couplers

机译:217单模光纤耦合器上光学测量的耗费217逆向比较

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Single-mode 2×2 optical fibre couplers have important applications in optical fibre networks, instrumentation and sensor systems. Bidirectional couplers made using the fused biconical taper technique are now provided by a large number of manufacturers. The transmission characteristics are inherently wavelength and polarization dependent, which may be of use for wavelength multiplexers and polarization splitters respectively, but is unwanted for optical power splitters [1]. The COST 217 project group decided in October 1988 to start a new Working Group (WG5) in order to develop measurement procedures for optical characterization of these and other branching devices. Up to now final agreement on such procedures is still lacking [2]. Like it was done in the other working groups [3], the 8 participants decided to start an interlaboratory comparison of measurements using different techniques. For this round robin 7 fibre couplers (named A to G) were circulated among the participants. The couplers, constructed with two identical 1300 nm single-mode fibres, were either 1300/1550 nm wavelength multiplexers or power splitters. After discussion of the first measurement results, the definitive experimental procedures were agreed on. These procedures as well as some experimental results are summarized in this paper. The definitions of the optical parameters of fibre couplers used in this paper are given in Figure 1. These properties can be measured as a function of wavelength and as a function of linear polarization angle with the degree of polarization of the light beam launched into the coupler to be 0 and 1 respectively. By rotating an analyzer in the beam, the maximum (I_(1)) and minimum (I_(2)) transmitted intensity can be determined. The degree of polarization P is then defined to be: P=(I_(1)-I_(2))/(I_(1)+I_(2)) (1)
机译:单模2×2光纤耦合器在光纤网络,仪表和传感器系统中具有重要应用。使用熔融双锥形技术制造的双向耦合器现在由大量制造商提供。传输特性是固有的波长和偏振,其可以分别用于波长多路复用器和偏振分离器,而是对光学电源分路器的不需要[1]。成本217个项目组在1988年10月决定开始新的工作组(WG5),以便开发用于这些和其他分支设备的光学表征的测量程序。现在,关于此类程序的最终协议仍然缺乏[2]。就像它在另一个工作组中完成的[3],8名参与者决定使用不同技术开始测量的互责任比较。对于这种循环7,罗宾7光纤耦合器(命名为G)在参与者之间流传。用两个相同的1300nm单模光纤构造的耦合器是1300/1550nm波长多路复用器或电源分路器。在讨论第一次测量结果后,达成了明确的实验程序。本文总结了这些程序以及一些实验结果。本文中使用的光纤耦合器的光学参数的定义在图1中给出。这些特性可以作为波长的函数测量,并且作为线性偏振角的函数,与发射到耦合器中的光束的偏振程度分别为0和1。通过在光束中旋转分析器,可以确定最大(I_(1))和最小(I_(2))发送的强度。然后定义偏振程度为:p =(i_(1)-i_(2))/(i_(1)+ i_(2))(1)

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