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Based on our computation, ε c = -1.2465.
Our computation of the PDFs is much less complicated than GFRD and more flexible.
Diffusive pathways are not a priori set but rather emerge naturally as part of our computation.
All our computation occurs on the surface, rather than in the voxel grid.
Our computation shows that conveyor malfunction is the prime factor for breakdown in CLG section.
In our computation, all the residual errors are less than (1.0times10^{-7}).
Nevertheless, we are here most interested in discussing the possible diffusion contribution to our computation results.
We also check our computation by the inverse integrating factor method.
This is based on our computation of the data we present in the next section.
In our computation, we find solutions at different time levels for various decreasing values of ε.
A basicenergy identity for anticipative stochastic integralswill be obtained as a byproduct of our computation of curvature.
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