By continuing this procedure, we can obtain images of the microstructures as a function of depth with a 4-nm lateral resolution and a 10-nm depth resolution.
Following analogous procedure, we can obtain the same observations as in the Observations 1 and 2 for DT and OWRT.
end{aligned} (21e) Following the same procedure, we can obtain the next higher-order continuity equation and (z) component of momentum equation as, i.e. (O epsilon ^4)).
According to the above procedure, we can obtain 2 28 candidates of the following 56-bit round key by using one random nibble fault injected to I 29, 7 L. (1) Round 29: K 29,7.
Remark 5.3 Using the same procedure, we can obtain similar results for equation (1.1) on the semiaxis R + with boundary conditions u ( 0 ) = d 2 u ( 0 ) d t 2 = 0 or d u ( 0 ) d t = d 2 u ( 0 ) d t 2 = 0.
The applicability is tested on the Lorenz model, where it is shown that by following the proposed procedure one can obtain asymptotic regulation quite well in the presence of unmodeled dynamics.
Finally, switch to system (2.6) and move toward P + along I ( P + ) (for t ∈ [ t +, + ∞ ) ). With a similar procedure, we can obtain a heteroclinic trajectory from P + to P −. In fact, we can move by system (2.6) along O ( P + ) from P + to the intersection point of O ( P + ) with a closed curve external to P +, namely γ (for t ∈ ( − ∞, t − ] ).
After the filtering procedure, we can obtain highly reliable miRNA-target and protein-protein interaction networks.
Following the above procedure, we can obtain the Weibull distributions of m gene expressions, denoted by F(1)(x), F(2)(x),..., F(m)(x).
