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Wavelength calibration of an imaging spectrometer based on Savart interferometer

机译:基于Savart干涉仪的成像光谱仪的波长校准

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摘要

The basic principle of Fourier-transform imaging spectrometer (FTIS) based on Savart interferometer is outlined. The un-identical distribution of the optical path difference which leads to the wavelength drift of each row of the interferogram is analyzed. Two typical methods for wavelength calibration of the presented system are described. The first method unifies different spectral intervals and maximum spectral frequencies of each row by a reference monochromatic light with known wavelength, and the dispersion compensation of Savart interferometer is also involved. The second approach is based on the least square fitting which builds the functional relation between recovered wavelength, row number and calibrated wavelength by concise equations. The effectiveness of the two methods is experimentally demonstrated with monochromatic lights and mixed light source across the detecting band of the system, and the results indicate that the first method has higher precision and the mean root-mean-square error of the recovered wavelengths is significantly reduced from 19.896 nm to 1.353 run, while the second method is more convenient to implement and also has good precision of 2.709 nm.
机译:概述了基于Savart干涉仪的傅里叶变换成像光谱仪(FTI)的基本原理。分析了导致每行干涉图的波长漂移的光路径的不相同分布。描述了呈现系统的波长校准的两个典型方法。第一方法通过具有已知波长的引用单色光统一每行的不同光谱间隔和最大频谱频率,并且还涉及Savart干涉仪的色散补偿。第二种方法基于最小二乘拟合,通过简明方程构建回收波长,行数和校准波长之间的功能关系。通过在系统的检测带上通过单色光和混合光源进行实验证明这两种方法的有效性,结果表明第一方法具有更高的精度,并且恢复波长的平均根平均误差是显着的从19.896 nm降至1.353运行,而第二种方法更方便实施,并且还具有2.709 nm的良好精度。

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