Abstract

Geometrical symmetry is found in many linear field problems. Group representation theory is the only valuable tool for exploiting this property from a computational point of view. In this context, here we apply a technique for taking into account equivariance in the numerical treatment of space–time boundary integral equations, which are invariant under a finite group G of congruences of R 3 , each related to one of the so-called Platonic solids. This technique is based upon suitable restriction matrices strictly related to a system of unitary, irreducible, pairwise not-equivalent matrix representations of G . The main development is expounded in the framework of space–time energetic boundary element method applied to Neumann exterior wave propagation problems, where the discretization matrices have a block lower triangular Toeplitz structure, and the diagonal block, to be inverted at each time step, is typically dense. Several numerical results, related to computational saving, are presented.

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