I am wondering if it is possible to have a continuum of bound states in a finite system, for example a molecular system with a fixed number of nuclei and electrons. As a chemist, I'm used to discussions that are limited to discrete bound states, so I never thought about the possibility of a continuous spectrum of bound states besides unbound states above the ionization limit.
So my question is is whether there can be a continuous spectrum of bound states in an operator of the type
$$ \hat H = \hat T + \hat V $$ where $\hat T$ is the sum of all kinetic energy operators for all particles and $\hat V$ is a Coulomb potential operator for all involved particles. The system is not allowed to be a crystal with translational symmetry. It is a finite system. Let us also assume that we disregard the translation of the center of mass and the associated states. Consider this "total translation" to be separated such that only internal degrees of freedom remain.
This question was sparked by a review of the Born-Oppenheimer approximation, where one often encounters the claim that any molecular wavefunction can be expanded into a sum of the form $$ \psi(r,R) = \sum_n\theta_n(R)\varphi_n(r;R), $$ where $\theta_n(R)$ is the nuclear wavefunction and $\varphi_n(r;R)$ is an electronic eigenfunction of the associated electronic clamped-nuclei Hamiltonian. It is not clear why there shouldn't be continuous states involved in such an expansion, but in all the sources, that are known to me, I have never encountered a discussion of this point.