Abstract
The Faddeev technique is employed to address the problem of describing the influence of both particle-particle and particle-hole phonons on the single-particle self-energy. The scope of the few-body Faddeev equations is extended to describe the motion of two-hole-one-particle (two-particle-one-hole) excitations. This formalism allows one to sum both particle-particle and particle-hole phonons, obtained separately in the random phase approximation. The appearance of spurious solutions for the present application of the Faddeev method is related to the inclusion of a consistent set of diagrams. The formalism presented here appears practical for finite nuclei and achieves a simultaneous inclusion of particle-particle and particle-hole phonons to all orders while the spurious solutions are properly eliminated.
| Original language | English |
|---|---|
| Article number | 034313 |
| Pages (from-to) | 343131-3431312 |
| Number of pages | 3088182 |
| Journal | Physical Review C - Nuclear Physics |
| Volume | 63 |
| Issue number | 3 |
| DOIs | |
| State | Published - Mar 2001 |