“…In this section, we illustrate our results with the control of the interconnection of two systems governed by the 1D wave equation; see, for instance, [18]. The coupling is achieved by control laws involving distributed delays, which are well known to successfully address stabilization problems; see, for instance, [19] and the references therein. This interconnection is shown in Figure 1: The square gray nodes characterize pointwise and distributed delays with kernel in P C .OE0; r N /; R n /, while the other nodes of the network are dynamical systems of second-order linear hyperbolic partial differential equations @´´ k .´; t / 1 c 2 @ t t k .´; t / D 0; t > 0;´2 .0;`k/ (56)…”