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For both epoxy systems, the diffusion processes follow a pseudo-fickian behaviour with two diffusive stages.
Different structure defects may have different influence on diffusion processes.
Parameter T is crucial to switch the two diffusion processes.
This work develops Feynman-Kac formulae for switching diffusion processes.
These tracks are spread out through charge diffusion processes.
Appropriate tools used for SC discharge are diffusion processes.
Considering the effect of different parameters on the anomalous diffusion processes, we present the diffusion processes with several varied parameters in Figure 5.
However, some diffusion processes, especially in various complex systems, no longer follow Gaussian behavior.
In contrast, only certain periods of field experiments on paint B are controlled by diffusion processes.
As shown in Figure 3, the anomalous diffusion processes present different characteristics from the conventional diffusion.
Clearly, the smaller the orders are, the stronger the diffusion processes are.
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