Abstract
The calculation of resonances according to the definitions of Siegert and of Kapur and Peierls is illustrated for s waves of a single particle in a potential well. A variational principle incorporating outgoing-wave boundary conditions is used. It picks out a resonance from the continuum of unbound states and yields simultaneously both the resonance energy and the decay width.
The variational principle is applied to calculate the two simplest 2Σ+ electron resonances of the H2- ion, both of which go over into H + H- for large separations of the nuclei. For small separations they have the electronic configurations (1sσg)2(2pσu) 2Σu+ and (1sσg)(2pσu)2 2Σg+.