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Table 2 The ability of 2In loop to buffer TF noise under of parameters in all three models.

From: Dynamics of miRNA driven feed-forward loop depends upon miRNA action mechanisms

Parameter values

Stop Model

Degr. Model

Dual Degr. Model

 

ε ̄

n

ε ̄

n

ε ̄

n

h s = 1 h s = 100 h s = 200 h s = 400

- 0 . 50 - 0 . 65 - 0 . 81 - 0 . 84

0 0 0 0

- 0 . 49 - 0 . 5 7 - 0 . 54 - 0 . 48

0 0 0 0

- 0 . 48 - 0 . 54 - 0 . 5 6 - 0 . 52

0 0 0 0

k q = 0 . 02 k q = 0 . 04 k q = 0 . 08 k q = 0 . 16

- 0 . 82 - 0 . 82 - 0 . 56 - 0 . 35

0 0 0 9

- 0 . 71 - 0 . 53 - 0 . 44 - 0 . 33

0 0 0 13

- 0 . 76 - 0 . 56 - 0 . 39 - 0 . 33

0 0 5 14

k s = 0 . 01 k s = 0 . 25 k s = 0 . 50 k s = 0 . 75

- 0 . 47 - 0 . 73 - 0 . 8 2 - 0 . 71

0 0 0 0

- 0 . 48 - 0 . 5 7 - 0 . 54 - 0 . 51

0 0 0 0

- 0 . 49 - 0 . 51 - 0 . 56 - 0 . 57

0 0 0 0

h p ( h g ) = 30 ; k r s = 1 â‹… 1 0 - 5 h p ( h g ) = 60 ; k r s = 2 â‹… 1 0 - 5 h p ( h g ) = 120 ; k r s = 4 â‹… 1 0 - 5 h p ( h g ) = 240 ; k r s = 8 â‹… 1 0 - 5

- 0 . 65 - 0 . 8 1 - 0 . 74 - 0 . 57

0 0 0 0

- 0 . 48 - 0 . 54 - 0 . 57 - 0 . 53

0 0 0 0

- 0 . 53 - 0 . 55 - 0 . 58 - 0 . 63

0 0 0 0

  1. For each model and for each parameter value we present the average ε value (left column) and the number n of experiments with positive values of this coefficient (right column). The method for calculation of ε is described in section. Negative ε mean that TF noise is dampen in a loop. The extremal ε values achieved at intermediate parameter values are shown in bold. The Wilcoxon Rank-Sum Test was used to test for significance of difference between the ε values for adjacent parameter values. The differences which are statistically insignificant at the α = 0.05 level are placed in parentheses.