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One can calculate that ∑ C$_{kl}$ ∈ N$_{1}$ (1 , 1) C kl 11 = 0 . 17 , ∑ C$_{kl}$ ∈ N$_{1}$ (1 , 2) C kl 12 = 0 . 25 , ∑ C$_{kl}$ ∈ N$_{1}$ (1 , 3) C kl 13 = 0 . 12 , ∑ C$_{kl}$ ∈ N$_{1}$ (2 , 1) C kl 21 = 0 . 28 , C$_{kl}$ ∈ N$_{1}$ (2 , 2) C kl 22 = 0 . 38 , C$_{kl}$ ∈ N$_{1}$ (2 , 3) C kl 23 = 0 . 21 , C$_{kl}$ ∈ N$_{1}$ (3 , 1) C kl 31 = 0 . 19 , C$_{kl}$ ∈ N$_{1}$ (3 , 2) C kl 32 = 0 . 27 , ∑ C$_{kl}$ ∈ N$_{1}$ (3 , 3) C kl 33 = 0 . 18 . The conditions ( C 5) − ( C 7) are valid for (6.15) with γ$_{0}$ = 3 , µ = 0 . 38 , ¯ c = ¯ d = 0 . 25 / 3 , M = 0 . 005 , L = 0 . 1 , ¯ L = 0 . 35 , ¯ l = 0 . 34 / 3 . According to Theorem 5.1, the network (6.15) has a unique almost periodic solution, which is exponentially stable with the rate of convergence 3 / 2 . 

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Consider the constant function φ ( t ) = { φ$_{ij}$ ( t ) } such that φ$_{11}$ ( t ) = − 0 . 025 , φ$_{12}$ ( t ) = 0 . 036 , φ$_{13}$ ( t ) = − 0 . 014 , φ$_{21}$ ( t ) = 0 . 012 , φ$_{22}$ ( t ) = − 0 . 021 , φ$_{23}$ ( t ) = 0 . 042 , φ$_{31}$ ( t ) = 0 . 023 , φ$_{32}$ ( t ) = − 0 . 015 , φ$_{33}$ ( t ) = 0 . 012 . We depict in Figure 1 the solution x ( t ) = { x$_{ij}$ ( t ) } of (6.15) with x ( t ) = φ ( t ) , t ≤ σ = θ$_{0}$ = 1 4 . Figure 1 supports the result of Theorem 5.1 such that the represented solution converges to the unique almost periodic solution of SICNN (6.15). 

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