We consider Klein-Gordon equations with an external potential V V and a quadratic nonlinearity in 3 + 1 3+1 space dimensions. We assume that V V is regular and decaying and that the (massive) Schrödinger operator H = − Δ + V + m 2 H = - + V + m² has a positive eigenvalue λ 2 > m 2 ² > m² with associated eigenfunction ϕ. This is a so-called internal mode and gives rise to time-periodic and spatially localized solutions of the linear flow. We address the classical question of whether such solutions persist under the full nonlinear flow, and describe the behavior of all solutions in a suitable neighborhood of zero. Provided a natural Fermi-Golden rule holds, our main result shows that a solution to the nonlinear Klein-Gordon equation can be decomposed into a discrete component a (t) ϕ a (t) where a (t) a (t) decays over time, and a continuous component v v which has some weak dispersive properties. We obtain precise asymptotic information on these components such as the sharp rates of decay | a (t) | ≈ t − 1 / 2 |a (t) | t^-1/2 and <
Léger et al. (Fri,) studied this question.