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ZERO-DISPERSION WAVELENGTH MEASURING METHOD FOR OPTICAL FIBER

机译:光纤的零色散波长测量方法

摘要

PURPOSE:To obtain a high-accuracy measurement result by making light which has a continuous wavelength spectrum and is intense enough to generate nonlinear optical effect in an optical fiber incident onto an optical fiber to be measured from its one end. CONSTITUTION:Light pulses oscillated by a Nd.YAG laser 10 are made incident on one end of the optical fiber 11 and inductive Raman scattering is caused while the pulses are propagated in the optical fiber 11, thereby obtaining light pulses having the continuous wavelength spectrum. Then the projection light from the other end of the fiber 11 is made incident on one end of the optical fiber 12 to be measured, nonlinear optical effect, etc., is caused by this fiber 12, and the light is projected from the other end on a spectroscope 13 controlled by a control part 15. The projection light of this fiber 12 has its wavelength spectrum measured from the relation between the indication wavelength of the spectroscope 13 and the output of a photodetector 14. The wavelength with which the intensity decreases greatly as compared with other wavelength components with respect to the wavelength spectrum of the projection light is selected as the zero-dispersion wavelength of the fiber 11.
机译:目的:通过制作具有连续波长光谱且强度足以从一端入射到要测量的光纤的光纤中产生非线性光学效应的光来获得高精度的测量结果。组成:由Nd.YAG激光器10振荡的光脉冲入射到光纤11的一端,并且当脉冲在光纤11中传播时引起感应拉曼散射,从而获得具有连续波长光谱的光脉冲。然后,使来自光纤11另一端的投射光入射到要测量的光纤12的一端,由该光纤12引起非线性光学效应等,并且从另一端投射光。光纤12的投射光具有由光谱仪13的指示波长与光检测器14的输出之间的关系测量的波长光谱。强度大大降低的波长是该光纤12的投射光。与其他波长分量相比,相对于投影光的波长光谱,选择光纤11的零色散波长。

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