Eur. Phys. J. A 12, 285-304 (2001)
Quasiparticle-phonon interaction in non-magic nuclei
S. Kamerdzhiev1, 2, E. Litvinova3 and D. Zawischa11 Institut für Theoretische Physik, Universität Hannover, Appelstraße 2, D-30167 Hannover, Germany
2 State Scientific Centre Institute of Physics and Power Engineering, Bondarenko Sq. 1, 249020 Obninsk, Russia
3 Institute of Nuclear Power Engineering, Studgorodok 1, 249020 Obninsk, Russia
zawischa@itp.uni-hannover.de
(Received: 22 June 2001 / Revised version: 11 October 2001 Communicated by P. Schuck)
Abstract
A general microscopic approach to describe properties of excited states
in
non-magic nuclei is formulated. It is based on the consistent
use of the Green function method in Fermi systems with Cooper pairing.
The main attention is paid to even-even nuclei, but for odd nuclei with
pairing some important relations are obtained too.
The quasiparticle-phonon interaction which is introduced acts also in
the particle-particle channel and gives a quasiparticle-phonon
contribution to pairing.
When applied to the theory of giant
multipole
resonances, the approach includes all known sources of
resonance width,
i.e. QRPA configurations (which correspond to Landau damping in magic
nuclei), the single-particle con- tinuum (escape width) and more complex
configurations (spreading width). The
use of the Green
function method makes it possible to include consistently the ground-state
correlations induced by the
more complex configurations. In the approximation of the collective
phonon creation amplitude squared, which is considered in detail
here, these are the ground-state correlations caused by
two-quasiparticle-phonon configurations;
effects of these
correlations have been found earlier to be noticeable for magic nuclei.
Such a unified approach will give a reasonable description of the
giant
resonances' integral characteristics including their widths and
of some more delicate properties like fine structure and decay
characteristics. Physical arguments and earlier results of a similar
approach for magic nuclei allow to use the known parameters of the
Landau-Migdal non-separable interaction for all non-magic nuclei (except
the light ones). This means that the theory
developed is suitable for
realistic predictions of the properties of unknown nuclei including
unstable ones. The inclusion of the single-particle continuum allows to
consider also nuclei with separation energy near zero.
21.60.-n - Nuclear-structure models and methods.
21.30.-x - Nuclear forces.
24.30.Cz - Giant resonances.
© Società Italiana di Fisica, Springer-Verlag 2001