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ESR spectra of impact glasses from the Kara astrobleme (upper spectrum) and Ries crater (bottom spectrum): A – the full range spectra; B – magnified part region of g = 2.00.
The optical spectra of the specimens were then measured in two ranged values: (1) reflectance THz range spectra from 40 to 700 cm− 1 and (2) reflectance ultraviolet, visible, and near-infrared spectra from 250 to 2000 nm.
The comparative analysis of the in situ ESR and UV-vis-NIR (including low-energy NIR range) spectra of poly-[Ni(Schiff)] films recorded during their oxidation at ambient temperature was performed, which allowed us to monitor the formation of different charge carriers in the polymer at different doping levels and elucidate their structure as well as the extent of their delocalization.
The spectral ranges used for the glucose model were different from those used for fructose and sucrose, even though full range spectra were tested for all sugars.
It is thus necessary to develop new approach to fabricate high efficient sunlight-like WOLEDs considering broad range spectra and easy fabrication process, which are applied not only as perfect solar simulators [15 17] but also as an ideal daily lighting source.
Spectra (128 scans) were acquired at a 4 cm−1 resolution in the 4000 600 cm−1 range (spectra are not provided and will be included in a future paper dedicated to a more in depth characterization of the materials using destructive analysis).
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In this paper, we propose a multicast switching node architecture configured with limited range spectrum converter (LRSC) and full range spectrum converter (FRSC) for elastic optical switching node.
Figure 4 Range spectrum.
(b) The range spectrum result after compensation.
(a) The raw range spectrum of two point-like targets.
The raw range spectrum of the two point-like targets is shown in Figure 4a.
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