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Results show that, in both former and latter simulations, the new methods work better.
In these latter simulations, a proton bunch was successfully accelerated from 130 keV to about 36 MeV in a DWA with a length of 36.75 cm.
The maximum standard error from the latter simulations is then reduced from 0.707% to 0.500%.
These latter simulations examine the robustness of the estimation procedure to model violations.
The latter simulations separately consider the effects of E r and J d − s.
In the latter simulations counterion condensation arises naturally and responds to local charge densities with no approximations.
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From the latter model simulations it was concluded that ion diffusion and consequently ion decoupling can have significant effect on the mass transfer rate, although a rather special set of conditions is required.
We show the latter simulation in this paper.
The results showed that both new models performed better than the older ones in both former and latter simulation studies.
For instance, real GDP improves by US$269 million in the former, but US$340 million in the latter simulation (closure 1).
The latter simulation was carried out assuming pre-existing nuclei since the Cahn Hilliard model does not include any mechanism for nucleation.
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