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Figure 2 Raman spectra of the samples at different thickness of the Ni coating.
Figure 6 shows the typical relationship between reflection loss (RL) and frequency at different thickness.
Samples were plasma nitrided at different thickness of plasma surface layers.
The intensity ratios I(E2)/I(A2) for the ultrathin films at different thickness are shown in Table 2.
Electron beam evaporation technique of nanostructure coating has been used to prepare SiO2 film over Cu substrate at different thickness.
The magnetic properties of the films at different thickness have been studied somewhere else [11] exhibiting negligible changes on the magnetic properties when changing the film thickness.
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Fig. 1 a Simulated exit waves of Si at different thicknesses and zone axes.
Fig. 6 Reflection loss curves of a CoFe2O4 and b CoFe@C at different thicknesses.
GEANT4 code was applied to simulate the background radiation spectrum at different thicknesses of lead.
For accomplishing this, ZnO films were prepared by ALD at different thicknesses to obtain seed layers of different crystallographic nature.
AFM images of the evaporated deposition ITO films indicate changes in the surface behavior of the films at different thicknesses.
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