A comparison between data processing techniques for FTS based on high frequency interferogram sampling

计算机科学 采样(信号处理) 稳健性(进化) 振动 数字信号处理 解调 傅里叶变换 数据处理 离散傅里叶变换(通用) 信号处理 参考数据 快速傅里叶变换 计算 电子工程 算法 频道(广播) 声学 短时傅里叶变换 傅里叶分析 数学 计算机视觉 滤波器(信号处理) 计算机硬件 电信 工程类 物理 数学分析 操作系统 化学 基因 生物化学 数据库
作者
Roberto Panzeri,Bortolino Saggin,Diego Scaccabarozzi,Marco Tarabini
出处
期刊:Proceedings of SPIE 卷期号:10000: 100001F-100001F 被引量:1
标识
DOI:10.1117/12.2240346
摘要

This paper compares different data processing techniques for FTS with the aim of assessing the feasibility of a spectrometer leveraging on standard DAC boards, without dedicated hardware for sampling and speed control of the moving mirrors. Fourier transform spectrometers rely on the sampling of the interferogram at constant steps of the optical path difference (OPD) to evaluate the spectra through standard discrete Fourier transform. Constant OPD sampling is traditionally achieved with dedicated hardware but, recently, sampling methods based on the use of common analog to digital converters with large dynamic range and high sampling frequency have become viable when associated with specific data processing techniques. These methods offer advantages from the point of view of insensitivity to disturbances, in particular mechanical vibrations, and should be less sensitive to OPD speed errors. In this work the performances of three algorithms, two taken from literature based on phase demodulation of a reference interferogram have been compared with a method based on direct phase computation of the reference interferogram in terms of robustness against mechanical vibrations and OPD speed errors. All methods provided almost correct spectra with vibrations amplitudes up to 10% of the average OPD speed and speed drifts within the scan up to 20% of the average, as long as the disturbance frequency was lower than the reference signal nominal one. The developed method based on the arccosine function keeps working also with frequencies of the disturbances larger than the reference channel one, the common limit for the other two.
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