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Optical fiber interferometric spectrometer

机译:光纤干涉光谱仪

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摘要

We design an optical fiber spectrometer based on optical fiber Mach-Zehnder interferometer. In optical fiber Fourier transform spectrometer spectra information is obtained by Fourier transform of interferogram, which recording intensity change vs. optical path difference. Optical path difference is generated by stretching one fiber arm which wound around fiber stretch drive by high power supply. Information from detector is linear with time rather than with optical path difference. In order to obtain high accuracy wavenumber, reference beam is used to control the optical path difference. Optical path difference is measured by reference laser interference fringe. Interferogram vs. optical path difference is resampled by Brault algorithm with information from reference beam and test beam. In the same condition, one-sided interferogram has higher resolution than that of two-sided interferogram. For one-sided interferogram, zero path difference position must be determined as accurately as possible, small shift will result in phase error. For practical experiment in laboratory, position shift is inevitable, so phase error correction must be considered. Zero order fringe is determined by curve fitting. Spectrum of light source is obtained from one-sided interferogram by Fourier cosine transform. A spectral resolution of about ~3.1cm~(-1) is achieved. In practice, higher resolution is needed. This compact equipment will be used in emission spectra and absorption spectra, especially in infrared region.
机译:我们设计了基于光纤马赫曾德尔干涉仪的光纤光谱仪。在光纤中,傅立叶变换光谱仪通过干涉图的傅立叶变换获得光谱信息,记录了强度变化与光程差的关系。光程差是通过一根光纤臂伸长而产生的,该光纤臂通过高功率电源缠绕在光纤拉伸驱动器上。来自探测器的信息与时间呈线性关系,而不与光程差成线性关系。为了获得高精度波数,参考光束用于控制光程差。光程差是通过参考激光干涉条纹测量的。干涉图与光程差通过Brault算法使用参考光束和测试光束的信息进行重新采样。在相同条件下,单面干涉图的分辨率高于两面干涉图的分辨率。对于单侧干涉图,必须尽可能准确地确定零路径差的位置,小的偏移会导致相位误差。对于实验室的实际实验,位置偏移是不可避免的,因此必须考虑相位误差校正。零阶条纹由曲线拟合确定。通过傅立叶余弦变换从单侧干涉图获得光源的光谱。达到约〜3.1cm〜(-1)的光谱分辨率。实际上,需要更高的分辨率。这种紧凑的设备将用于发射光谱和吸收光谱,特别是在红外区域。

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