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The H2S loading in liquid phase decreases with the rising of absorption temperature under the same H2S partial pressure and the same component concentrations.
Meanwhile, the H2S partial pressure increases with the rising of absorption temperature at the conditions of a constant H2S loading and the same component concentrations of the aqueous absorption solution.
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Apart from the shift in the absorption edge, the optical properties of surface modified semiconductor nanoparticles, having a continuous rise of absorption toward higher energies, paralleled the absorption properties characteristic of the band structure in bare semiconductor nanoparticles.
The Abs spectrum of as-isolated CDO exhibits a shoulder at ∼21 750 cm–1 on a slowly rising background absorption above 12 000 cm–1 (see Figure 1).
94 Gratings with inclusions or indentations have been also considered to significantly rise the absorption of, for instance, organic materials.
The optical absorption spectrum of MoS2 nanocrystallines shows a minimum optical absorption feature of about 400 nm and strong rising absorption edge shifts towards the UV region.
The rise of light absorption is usually attributed to the increase of volume percentage of the semiconductor materials with high absorption coefficients.
Moreover, one can notice that the PL intensity significantly increases while n increases from 2.01 to 2.12, which is partly explained by the rise of the absorption.
It is evident that the rise of the absorption edge near the band edge for the pure ZnO nanorods (sample S1) increased gradually, while it becomes sharper for the Cu-doped ZnO nanorods (samples S2 to S5), indicating the presence of localized states within the bandgap.
The rise of the absorption band of FMN at λmax=445 nm obeyed first-order kinetics.
A rising absorption edge from 550 nm into the UV gives an evidence of the PSS-RGO-GeNPs.
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