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We study the notion of strong integrability for classically integrable -deformed CFTs and coset CFTs. To achieve this goal we employ the Poisson brackets of the spatial Lax matrix which we prove that it assumes the Maillet -matrix algebra. As a consequence the system in question are integrable in the strong sense. Furthermore, we show that the derived Maillet -matrix algebras can be realized in terms of twist functions, at the poles of which we recover the underlying symmetry algebras.

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