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Due to the global Lipschitz continuity of the coefficients of Eq. (5), one would expect that standard numerical methods such as the Euler Maruyama method are again geometrically ergodic for small enough step-sizes Δt (see [34], Theorem 7.3).
As discussed below, the results of the Real Time PCR method are again in excellent agreement with previous results obtained with other methods.
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The integrating matrix method is again applied to solve this nonlinear problem.
Secondly, in the numerical implementation the Shepard function method is again employed to construct a point-wise density interpolant.
Since this approach yields only a vague estimate of the true optimal shape of newly established holes, the traction method is again used for shape variation of the extended design boundary.
The proposed method is, again, faster than AHE.
Therefore, the SSplit method is again applied on subset "C" to identify the small edge.
The incremental method is again applied in [10] for stationary gas flow within a large decomposition framework.
Second, by fixing the mean structure, the forward stepwise method is again applied to determine the time lags for the sigma parameter in Eq. (6).
To answer these questions, the adjoint method is again the tool of choice, as it allows to compute a sensitivity map of the whole car for the positioning of jets.
The SR-ML method is again used in this example and the resulting fit is very close to the non-parametric cumulative incidence function as shown in Fig. 8-panel D. A further interest with the EBMT data in this article is to illustrate how the GLD fits could be improved and compared against well-known parametric models using mixture of Normal distributions.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com