• Title/Summary/Keyword: FTIR spectrometer

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Radiometric Calibration of FTIR Spectrometer For Passive Remote Sensing Application (수동형 원격탐지 FTIR 분광계의 Radiometric Calibration)

  • Kim, Dae-Sung;Park, Do-Hyun;Choi, Seung-Ki;Ra, Sung-Woong
    • Korean Journal of Optics and Photonics
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    • v.17 no.5
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    • pp.391-395
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    • 2006
  • In this paper, radiometric calibration of a FTIR spectrometer for passive remote sensing application was introduced and verified. Radiometric calibration is a significant signal processing procedure to retrieve the object radiance from the measured spectrum. The object radiance is measured and registered distorted by the detector's responsivity dependent on wavelength and instrument self-emission. Radiance of two temperature points, hot temperature and cold temperature, from a well-controlled blackbody was measured and used to obtain the scale factor and offset factor which are required for radiometric calibration. For gas phase C2H5OH. radiometric calibration was done and verified through comparison of its emission line width and intensity with the standard spectrum.

Fast Remote Detection Algorithms for Chemical Gases Using Pre-Detection with a Passive FTIR Spectrometer (수동형 FTIR 분광계에서 초동 탐지 기법을 이용한 고속 원거리 화학 가스 탐지 알고리즘)

  • Yu, Hyeonggeun;Park, Dongjo;Nam, Hyunwoo;Park, Byeonghwang
    • Journal of the Korea Institute of Military Science and Technology
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    • v.21 no.6
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    • pp.744-751
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    • 2018
  • In this paper, we propose a fast detection and identification algorithm of chemical gases with a passive FTIR spectrometer. We use a pre-detection algorithm that can reduce the spatial region effectively for gas detection and the candidates of the target. It is possible to remove background spectra effectively from measured spectra with the least-squares method. The CC(Correlation Coefficients) and the SNR(Signal-to-Noise Ratio) methods are used for the detection of target gases. The proposed pre-detection algorithm allows the total process of chemical gas detection to be performed with lower complexity compared with the conventional algorithms. This paper can help developing real-time chemical detection instruments and various applications of FTIR spectrometers.

Research on Far-Infrared Optical Spectra of Blood Substrates using FTIR-spectrometer (FTIR Spectrometer를 이용한 혈중성분의 원적외선 분광 스펙트럼에 관한 연구)

  • 김건식;전계진;윤길원;박승한
    • Proceedings of the Optical Society of Korea Conference
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    • 2000.02a
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    • pp.152-153
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    • 2000
  • 혈중 성분, 또는 생체 시료와 빛의 상호작용에 관한 연구는 비침습적 정량분석의 가능성을 의미하므로 많은 연구가 진행되고 있다. 특히 원적외선 검출소자가 급속히 개발됨에 따라 원적외선(8~15$mu extrm{m}$)영역에서의 생체 시료 및 성분들의 정량적인 분석과 영상에 관한 연구가 큰 주목을 받고 있으며, 그중 혈중 Glucose 성분의 정량분석에 관한 연구등은 여러 분광법으로 활발히 연구되고 있다$^{(1)(2)}$ . 본 연구에서는 혈중성분인 Glucose, Hb, Albumin을 수용액 상태로 원적외선 영역에서 흡수 specrtrum을 측정하여 정량분석에 대한 가능성을 확인하였다. (중략)

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Simulation for Small Lamellar Grating FTIR Spectrometer for Passive Remote Sensing

  • Chung, You Kyoung;Jo, Choong-Man;Kim, Seong Kyu;Kim, In Cheol;Park, Do-Hyun;Bae, Hyo-Yook;Kang, Young Il
    • Journal of the Optical Society of Korea
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    • v.20 no.6
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    • pp.669-677
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    • 2016
  • A miniaturized FTIR spectrometer based on lamellar grating interferometry is being developed for passive remote-sensing. Consisting of a pair of micro-mirror arrays, the lamellar grating can be fabricated using MEMS technology. This paper describes a method to compute the optical field in the interferometer to optimize the design parameters of the lamellar grating FTIR spectrometer. The lower limit of the micro-mirror width in the grating is related to the formation of a Talbot image in the near field and is estimated to be about $100{\mu}m$ for the spectrometer to be used for the wavelength range of $7-14{\mu}m$. In calculating the far field at the detection window, the conventional Fraunhofer equation is inadequate for detection distance of our application, misleading the upper limit of the micro-mirror width to avoid interference from higher order diffractions. Instead, the far field is described by the unperturbed plane-wave combined with the boundary diffraction wave. As a result, the interference from the higher order diffractions turns out to be negligible as the micro-mirror width increases. Therefore, the upper limit of the micro-mirror width does not need to be set. Under this scheme, the interferometer patterns and their FT spectra are successfully generated.