Table 1 The topological entropy $\mathit{h}\mathbf{(}\mathbf{Y}\mathbf{)}$ of constant CNNs with 2-components and templates being given by $\mathbf{(}{\mathbb{T}}_{\mathbf{1}}\mathbf{,}{\mathit{z}}_{\mathbf{1}}\mathbf{)}\mathbf{=}\mathbf{(}\mathbf{[}\mathbf{-}\mathbf{4}\mathbf{,}{\mathit{a}}_{\mathbf{1}}\mathbf{,}\mathbf{2}\mathbf{]}\mathbf{,}{\mathit{z}}_{\mathbf{1}}\mathbf{)}$ and $\mathbf{(}{\mathbb{T}}_{\mathbf{2}}\mathbf{,}{\mathit{z}}_{\mathbf{2}}\mathbf{)}\mathbf{=}\mathbf{(}\mathbf{[}\mathbf{-}\mathbf{2}\mathbf{,}{\mathit{a}}_{\mathbf{2}}\mathbf{,}\mathbf{-}\mathbf{4}\mathbf{]}\mathbf{,}{\mathit{z}}_{\mathbf{2}}\mathbf{)}$

From: Inhomogeneous lattice dynamical systems and the boundary effect