Abstract

Starting with all the electrons and nuclei making up a system of three atoms, we introduce a basis of antisymmetrized products of atomic states to define a matrix Hamiltonian partition applicable to atom–diatom collisions. We derive a three-atom generalization of the Faddeev equations in terms of diatomic transition operators. Equations are obtained for three-atom rearrangement transition operators that are then reduced to sets of effective two-body (atom–diatom) equations by introducing separable expansions of the diatomic transition operators. We also discuss the permutational symmetry of identical nuclei and briefly describe how the formalism applies to the H3 and FH2 systems.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.