Abstract
The existence of individual low-energy E1 toroidal and compression states (TS and CS) in Mg was predicted recently in the framework of quasiparticle random-phase-approximation (QRPA) model with Skyrme forces. It was shown that the strong axial deformation of Mg is crucial to downshift the toroidal strength to the low-energy region and thus make the TS the lowest E1(K=1) dipole state. In this study, we explain this result by simple mean-field arguments. Comparing TS in two strongly axial nuclei, Mg and Ne, we show that the lowest TS is not not a universal phenomenon but rather a peculiarity of Mg. The spectroscopy of TS and CS is analyzed and some additional interpretation of these states is suggested.
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