2011
DOI: 10.1016/j.cnsns.2010.08.010
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Dynamical behavior of the activator–repressor circuit model under random fluctuations

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Cited by 4 publications
(5 citation statements)
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“…Nevertheless, we have managed to calculate these deterministic quantities by accurate and efficient numerical methods. 13,[31][32][33][34][35] The noise intensities σ k , σ s , ε k , ε s , the Lévy motion index α (relating with the jump magnitude and its frequency) have important and subtle influences on MFET and FEP. We have used the relative contribution factor (RCF) λ , the ratio between non-Gaussian and Gaussian noise strengths, to implement optimal control in the transition between the two states, when the total quantities of the noise intensities are fixed.…”
Section: Discussionmentioning
confidence: 99%
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“…Nevertheless, we have managed to calculate these deterministic quantities by accurate and efficient numerical methods. 13,[31][32][33][34][35] The noise intensities σ k , σ s , ε k , ε s , the Lévy motion index α (relating with the jump magnitude and its frequency) have important and subtle influences on MFET and FEP. We have used the relative contribution factor (RCF) λ , the ratio between non-Gaussian and Gaussian noise strengths, to implement optimal control in the transition between the two states, when the total quantities of the noise intensities are fixed.…”
Section: Discussionmentioning
confidence: 99%
“…50 Then the generator A is Secondly, the AMFET on D is defined as ū(D) = 1 |D| D u(k, s)dkds for our analysis from the macroscopic perspective. 6,35 First escape probability (FEP) and average first escape probability (AFEP). The escape probability here are employed to characterize the likelihood of the transition between the low vegetative and the high competence region for the MeKS system.…”
Section: /13mentioning
confidence: 99%
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