Influence of Neutron-Core Excitations on High-Spin States in 88Sr S
E.A. Stefanova1, R. Schwengner, J. Reif, H. Schnare, F. Dönau, M. Wilhelm2, A. Fitzler2, S. Kasemann2, P. von Brentano2, and W. Andrejtscheff1

High-spin states of the N = 50 nucleus 88Sr were studied via the reaction 80Se(11B,p2n) at a beam energy of 45 MeV with the six-detector array OSIRIS CUBE at the University of Cologne. The level scheme of 88Sr deduced from this experiment is shown in Fig. 1. On the basis of the analysis of directional correlations of coincident g rays emitted from oriented states (DCO), spin assignments for all observed states were made. Mean lifetimes of three levels were determined using the Doppler-shift-attenuation method. They correspond to strong M1 transitions with B(M1) values of about 0.3 to 1.4 W.u. Shell-model calculations in the model space (0f5/2, 1p3/2, 1p1/2, 0g9/2) for the protons and (1p1/2, 0g9/2, 1d5/2) for the neutrons were performed. Experimental and calculated level energies of states in 88Sr are compared in Fig. 2. Neutron-core excitations are predicted for the lowest 6+ and 7+ states in agreement with results of previous (d,p) experiments (e.g. [1]). Proton configurations of seniority u = 4 are predicted for the positive-parity states with Jp = 8+, 10+, 11+ and 12+. The calculations describe experimental high-spin level sequences with Jp > 7- and Jp ³ 12+ linked by strong M1 transitions as u = 4 and 6 multiplets, respectively, which include proton excitations coupled to neutron-core excitations. A detailed description of this work is given in Ref. [2].

stefanova1.gif

Fig. 1 Level scheme of 88Sr deduced from the present experiment.

stefanova2.gif Fig. 2 Comparison of experimental with calculated level energies in 88Sr.

1 FZR and Institute for Nuclear Research and Nuclear Energy, BAS, 1784 Sofia, Bulgaria
2 Institut für Kernphysik, Universität zu Köln, 50937 Köln, Germany

References

[1] P.C. Li et al., Nucl. Phys. A 462 (1987) 26
[2] E.A. Stefanova et al., Phys. Rev. C 62 (2000) 054314

FZR
 IKH 06/22/01 © E. A. Stefanova