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We describe the propagation of singularities of tempered distributional
generalized eigenfunctions of many-body Hamiltonians at non-threshold energies
under the assumption that the inter-particle interactions are real-valued
polyhomogeneous symbols of order -1 (e.g. Coulomb-type, but without the
singularity at the origin). Here the term singularity' refers to a microlocal description of the lack of decay at infinity. We use this result to describe the wave front relation of the S-matrices. We also analyze Lagrangian properties of this relation, which shows that the relation is not too large’
in terms of its dimension.

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