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When using a microPET scanner with a long axial-FOV, such as Inveon for small animals, the main scatter source is located inside the FOV.
This is introduced because stationary targets can have high speeds because they fluctuate in the position because of measurement uncertainty or the main scatter points are moving, i.e., wind turbine.
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A decrease of 2DEG mobilities limited by three main scattering mechanisms, including misfit dislocation, threading dislocation and interface roughness scatterings, is observed with increasing value of the density of interfacial charges.
Therefore, our data suggest that Coulomb scattering is the main scattering mechanism in our device.
This linear dependence gives indication on the main scattering mechanisms limiting l in our graphene samples.
The main scattering mechanism in the thin ZnO Ti films was defect scattering.
The main scattering mechanisms in one- to three-layer graphene are Coulomb scattering [21 23], short-range scattering [24] and phonon scattering by graphene phonon [25].
In both cases, the disorder coming from the boundary scattering plays the fundamental role giving the main scattering mechanism for the diffusive electron transport.
In order to take into account the main scattering process we calculate ionized impurities scattering as a function of magnetic field.
Hence, charged impurities, either adsorbed on graphene surface, or located at the interface with SiO2 substrate, can be assumed as the main scattering source liming l.
At low temperature, the main scattering mechanisms in graphene are largely due to the Coulomb impurity and the short-range defect scatterings [24].
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