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For the magnetron sputtered films, the D peak broadened, the broadening being proportional to ordering in the films.
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Hence, using the Lorentz and van der Waals broadenings, the Stark broadening is calculated.
Natural broadening is always present, is the same at all wavelengths, and is very small.
The way this broadening is implemented is also important.
CTZ band broadening was observed with ratio 50% (Table 2).
Peak broadening was modelled using a Lorentzian crystallite size term.
Moreover, residues with significant exchange broadening are found.
The line broadening is essentially due to the size effect.
Moreover, the chromatography peak broadening was greatly compressed.
The broadening is 131.42 meV for the second peak.
This peak broadening was caused by a smaller crystallite size.
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