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It emphasizes to introduce a variety of essential components for constructing hyperspectral imaging systems, including light sources, wavelength dispersion devices, and detectors.
Related instruments for constructing and calibrating scanning imaging systems, such as light sources, wavelength dispersion devices, detectors, standard test charts, calibration sources, and standard reflectance panels, are already commercially available.
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The polymers doped with chlorinated dopants showed no absorption peak and retained the broad windows around the source wavelength.
The spectra were recorded in air at room temperature using a 17 mW He-Ne laser source (wavelength 632.8 nm).
However, the related investigation techniques rely either on pure electrochemical techniques regardless of the light source wavelength either on photochemical processes with a poor electrochemical description.
The treatment efficiency of the system was evaluated by varying the hydraulic retention time (HRT), light source wavelength, and quantity of photocatalyst.
This allows constraints to be relaxed on source wavelength accuracy and passive filter selectivity, and also alleviates power and area issues by reducing the number of active devices.
For this purpose, a water penetrable laser source (wavelength ~ 532 nm) was operated at two power densities (6 and 9 GW cm− 2).
Raman laser was used at an excitation source wavelength of 532 nm, the Raman analysis was carried out using dispersive Raman spectroscopy, Senterra, Bruker, Germany.
The crystal structure of the prepared films was analyzed by X-ray diffraction (XRD) with CuKα1 radiation (source wavelength is 1.5406 Å).
Also, the incident angle of the laser source can be tuned precisely, 0.01°, in order to find an incident angle that matches between the laser source wavelength and the resonance wavelength of the PC-based nanofluidic channels.
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