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Figure 2 shows UV spectra exposed from the reaction of reduction of silver ions which have polydispersed nanoparticles with broadening peak in the absorbance band at the wavelength of 450 nm.
As in the case for the saturation time, the broadening peak time is dependent on beta: the peak time is increasingly delayed with higher values of beta.
From the broadening peak at 2θ = 51.8°, the particle metallic size are lower for Ni(n w), Ni(a w) and Ni(n e) samples.
The broadening peak at 3460 cm−1 for G GA and 3468 cm−1 for graphite meanwhile is originating from the presence of hydrogen bonded OH groups in both samples.
It can be seen that increasing the temperature up to 1,000°C causes a decrease in intensity of this broadening peak, which is due to evaporation of organic compounds and water from the powders.
At a higher value of beta (β i=0.2), the order is reversed and the broadening peak time arrives approximately 50 gyroperiods after the saturation of linear-mode fluctuations.
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The weak and broadened peak at 25° to 28° can be assigned to the carbon (002).
The broaden peak from 1,100 to 1,700 cm-1 demonstrates the existence of amorphous carbon structure [45].
The Co-doped WS2 nanorods, however, show significantly broadened peak shapes, indicating that the crystallite size is much smaller than that of the raw WS2 powder.
Preliminary studies have also shown that the relaxed structure usually accompanies with the broadened peak of (112) orientation, which is associated with high degree of structural disorder[14].
The nearly constant integrated areas under the CO-stripping CV peaks and broadened peak shapes indicate a stable number of Pt/Ru bimetallic alloy surface sites, yet the surface composition distribution is broadened.
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CEO of Professional Science Editing for Scientists @ prosciediting.com