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On the other hand, the carbon dioxide corrosion of mild steel in the presence of acetate also detected the Bragg diffraction peaks for Fe2(OH)2CO3 and Fe2O2CO3; however, the α-Fe diffraction peaks of the underlying steel substrate were not extinguished with time, and there was a reversal in the pattern of evolution of the intensities of the Fe2(OH)2CO3 and Fe2O2CO3 phases in acetate.
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The temporal evolution of the intensity of fluctuating energy is investigated by analyzing the most dominant mode in the system.
The evolution of the intensity ratio between the G band (1585 cm−1) and the disorder-induced D band (1345 cm−1) with ion dose is determined, providing a spectroscopy-based method to quantify the density of defects in graphene.
The evolution of the intensity ratio between the parallel polarized D band (VV) and the perpendicular polarized D band (VH) is determined, providing a spectroscopy-based method to probe the atomic scale edge structures in graphene.
The evolution of the intensity of Ti K-edge pre-edge peak gives evidence of the incorporation of Ti in hexagonal lattice of AlN for Al-rich films and in cubic lattice of TiN for Ti-rich films.
We studied the mixing using tracer particles for the completely and partially filled states, evaluated the time evolution of the intensity of segregation and fitted kinetic laws in order to determine mixing rates.
The evolution of the intensity of the C1s components is reported in Fig. 12.
Figure 5 b shows similarly the evolution of the intensity (top) and activation time (bottom) estimates with each pairwise exchange.
Briefly, in DLS measurements, the temporal evolution of the intensity fluctuations of visible light that travels a known distance through an aqueous suspension is used to measure the translational diffusion coefficients of suspended colloids/particles.
Similarly, Figs. 7 c and 8 c show the evolution of the intensity (top) and activation time (bottom) estimates with increasing number of pairwise message exchanges, for K=1 and K=5, respectively.
In this paper, we present a detailed study of the evolution of the intensity of the magnetic moment per Co atom (either FM or AFM) on Co-doped SnO2 thin films sputtered on SiO2/Si 001) substrates at RT followed by thermal treatments in vacuum under magnetic field applied out-of-plane and in-plane configurations.
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