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Figure 2 shows the FTIR spectrum of the sample, the absorption peak at 587 cm−1 identified vibration of γFe-O [35, 36], and the other peaks at pure maghemite are 454, 632, 795, 892 cm−1.
For each sample the absorption at 420 nm and 550 nm was recorded and the mean activity was obtained from four independent measurements.
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In several samples, the absorption factor was not in the range 1.5 5.
Meanwhile, for the CQD-modified samples, the absorption intensity increased with the CQD content increase.
In bulk samples, the absorption signal is an average of all coordination environments of a particular element.
In the IR spectrum of the samples, the absorption band at 3700 3500 cm−1 is due to vibrations of OH bonds on the surface of TiO2.
The absorption edge of bulk CdS is at 515 nm (2.43 eV); while in our prepared samples the absorption peak position is observed at 477, 463, and 450 nm for 1, 2 and 5 wt% co-dopant concentration, respectively.
With T c rise (in the range of 500 700 °C) for Cu-8 samples, the absorption band at ~270 nm intensifies indicating an increase in the number of oxygen vacancies in the nanocrystals.
For sample c and sample d, the absorption of light energy was greater than the silicon wafer in 350 to 1,000 nm, but it was increased tremendously up to 83% in 200 to 350 nm.
For individuals in the second group, fasting blood samples were collected by venepuncture at approximately 08.00 hours on day 3 (corresponding to the 48 h sample in the absorption group), 4, 5, 6, 9, 12, 18 and 21.
The CoSb3-NON sample indicates the absorption peak maximum at about 640 nm.
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