In the current work a setup for the acquisition of high resolution multispectral, spectroscopic mapping infrared images is presented. The idea is based on the Fourier Transform Infrared (FTIR) reflectoscopy since the object is illuminated using the source and the interferometer of an FTIR spectrophotometer and the reflected signal intensity from the object is measured using a high resolution response of a Focal Plane Array (FPA) of InSb sensor. The optical parts like optical fibers, mirrors, beamsplitters, FPA and the FPA lens are selected properly to allow the measurement at a wide frequency range depending on the spectral range of the source interferometer from wavelength 1.3 μm to 26 μm and the spectral range of the FPA which in this case is from wavelength 1.3 μm to 5.5 μm and beyond but with significant attenuation. Moreover, the FPA is triggered through the laser signal that measures the position of the moving mirror of the interferometer and by adjusting appropriately the speed of the scanner mirror and the FPA integration time, the array of interferogramms of a significant region of interest (ROI) can be acquired instantly. This is one of the main contributions of the present work since multispectral images in a non-micrometer level and from an area of a few centimeters by centimeters are acquired by extracting the interferogram, through each sensor of the FPA, in the illuminated ROI and in a time interval less than 1 sec. This is providing to the user the fast acquisition mapping images in a wavelength resolution of the order of less than manometer (based on the spectrophotometers resolution) in a broadband area as stated before. This kind of mapping, multispectral cube images with sub nanometer spectral interval among them, up to now, are acquired by scanning point by point, in an array format, in a ROI of 2 cm by 10 cm, lasting approximately 8.8 hours with 16 averaging per signal. By using this technology in the field of heritage science, the scientists can simultaneously observe, in the case of painted artworks like the ones presented in this manuscript, the overpaintings, pentimenti, defects in the underlayers based on the cube imaging, produced data set, as well as materials identification based on the spectra that are acquired per pixel simultaneously to the cube imaging data set. Using the iTomography system and applying mosaic scanning, the acquisition time of spectroscopic mapping cube images from the hole object, like the icon presented in this work, with dimensions 60 cm × 70 cm, is of the order of 8-10 minutes.
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