Abstract
The standard Random Phase Approximation (RPA) is extended by including the exchange of one- and the coupling to two-phonon excitations in the residual interaction. Within this scheme a microscopic understanding of the excitation spectra of doubly closed-shell nuclei, like e.g. 16O, is possible. The mechanism to generate the many low-lying isoscalar natural parity states in 16O is discussed and related to the attraction of the residual nucleon-nucleon (NN) interaction. The connection of this residual particle-hole (ph) interaction with the treatment of the single-particle (sp) self-energy is discussed.
This research was supported in part by the Condensed Matter Theory Program of the Division of Materials Research of the U.S. National Science Foundation under Grant No. DMR-8519077 and in part by the U.S. Army Research Office.
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© 1988 Plenum Press, New York
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Dickhoff, W.H. (1988). The Particle-Hole Interaction in Finite Nuclei. In: Arponen, J.S., Bishop, R.F., Manninen, M. (eds) Condensed Matter Theories. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-0971-0_23
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DOI: https://doi.org/10.1007/978-1-4613-0971-0_23
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