Abstract
AbstractThe yrast band in the heavy $$N = Z$$
N
=
Z
nucleus $$^{88}$$
88
Ru is studied in the framework of the $$\alpha $$
α
-cluster model in combination with double-folding potentials. It is found that the excitation energies of the yrast band in $$^{88}$$
88
Ru can be nicely described within the $$\alpha $$
α
-cluster approach using a smooth and mildly L-dependent adjustment of the potential strength. This result is similar to well-established $$\alpha $$
α
-cluster states in nuclei with a (magic core $$\otimes $$
⊗
$$\alpha $$
α
) structure. Contrary, the yrast bands in neighboring $$N \ne Z$$
N
≠
Z
nuclei deviate from such a typical $$\alpha $$
α
-cluster behavior. Finally, the $$\alpha $$
α
-cluster model predicts reduced transition strengths of about 10 Weisskopf units for intraband transitions between low-lying states in the yrast band of $$^{88}$$
88
Ru.
Funder
New National Excellence Program of the Ministry of Human Capacities of Hungary
Nemzeti Kutatási Fejlesztési és Innovációs Hivatal
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
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