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The difference between the condition solution and the simple mean is provided in Fig. 2(b).
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(b) Difference between the condition adjustment solution and simple mean.
These input constraints were constant for each perturbation and comparative wild-type condition such that the calculated solution spaces between the conditions differed based only on variations in the output secretion constraints.
So the process puts the artist into the conditions where solutions unexpectedly appear.
It should be noted that even under the steady-state conditions the concentration difference between the drop solution and the environment solution is maintained (see Figure S6).
has the extremal solutions between the lower solution σ 1 ≡ − 1 and the upper solution σ 2 ≡ 1. Conditions (H1) through (H3) in Corollary 1.1 are obviously satisfied.
Lemma 1 reveals the relationship between the existence condition of JGMD and the solution of a constraint equation for two complex-valued matrices.
Theorem 4.2 shows that, under some conditions, the distance between the solution (X t)=(S t),I t),V t))) and the endemic equilibrium (P^=(S^,I^,V^)) of system (1.1) has the following form: limsup_{trightarrowinfty}frac{1}{t}int_{0}^{t} bigl| X s -P^bigr| ^{2},dsleqslant C|sigma |^{2}, quadmboX s -P^bigrere C is a positive constant.
(18) As the analogy of non-specific hybridization with the probes we estimate Kbulk, assuming that the free energy of bulk hybridization is proportional to that of non-specific hybridization Δ Gbulk = wbulk Δ Gns, where wbulk is an adjustable parameter which represents the difference of hybridization condition between solution and the array surface.
Moreover, the solution satisfies the condition (3.4).
This solution satisfies the condition (2).
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