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The results in this table show that with few numbers of retained modes we obtained a maximum pointwise error of order 10−8.
In Table 2, we list the maximum pointwise error E and the time elapsed τ for different values of M. The results in this table show that with few numbers of retained modes we obtained a reasonable accuracy 10−13.
Table 2 shows the elementary flux modes we obtained.
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Summing up for all the modes, we obtain the following log-likelihood function of the posterior distribution: L = ∑ n log p U n | M × ̄ n U n ∝ − ∑ n Ī n S 2 log | G n | + tr G n − 1 S n. (31).
Using k=20 for CLARK (full mode) we obtained a similar sensitivity to NBC (CLARK is actually more sensitive than NBC on HiSeq and simHC.20.500).
By further analyzing intracellular tubulin polymerization kinetics, cell cycle G2 population arrest, and cell viability in dose response mode, we obtained a comprehensive understanding of the drugs' intracellular mechanisms of action at a molecular level.
Therefore, by applying the exponential approximation for every r-mode, we obtain that (14).
Neglecting the decoupled mode, we obtain the equivalent model in which a quantum dot is coupled to a single lead.
We specially highlight that in the pulsed plasma mode, we obtain quantum-sized free standing alloy nanocrystals with a mean size of 7.3 nm.
By analyzing the formulae for the failure-modes we obtain piecewise defined functions describing the optimal cross-section and the minimum mass of the tube.
For the first EOF mode (EOF1), we obtained a pattern related to the summer rainy season.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com