Abstract
Low-energy dipole excitations in ${}^{10}$Be were investigated based on the generator coordinate method with $\alpha + {}^6$He and $\alpha + \alpha + 2n$ cluster models. We obtained three $1^-$ states in $E_{x} < 15$~MeV, which show different characters in the $E1$, compressive dipole, and toroidal dipole transition strengths. We found the strong toroidal dipole transition in the $1_1^-$ state, remarkable $E1$ strength in the $1^-_2$ state, and the strong $E1$ and compressive dipole strength in the $1^-_3$ state. The $1^-_1$ is described by the $\alpha + {}^6$He cluster structure, where as the $1^-_2$ and $1^-_3$ states are understood by three-body excitations of the $\alpha + \alpha + 2n$ clustering.
Highlights
In the dipole excitations of nuclei, significant low-energy dipole (LED) strengths have been observed in the energy region below the giant dipole resonance (GDR)
The significant LED strengths may indicate emergence of possible new excitation modes different from the GDR modes, which are usually understood by the collective oscillations of the whole system such as the proton–neutron incoherent oscillation for the IV-GDR and the compressive dipole oscillation for the IS-GDR
In our recent works with antisymmetrized molecular dynamics (AMD), we have studied the LED in light nuclei such as 10 Be [38] and 12 C [39], and predicted the toroidal dipole excitations
Summary
In the dipole excitations of nuclei, significant low-energy dipole (LED) strengths have been observed in the energy region below the giant dipole resonance (GDR). Cluster structures can contribute to the low-energy ISD excitations in light nuclei because the ISD operator, which is the compressive type with the r 3 term, can directly excite the inter-cluster motion as pointed out by Chiba et al in a similar way to the IS monopole excitations with the r 2 term [40,41,42,43] This means that the cluster excitation mode can be another candidate for the LED excitations. In the present calculation we apply the generator coordinate method (GCM) using α + 6 He and α + α + 2n cluster model wave functions in order to clarify details of two-body and three-body cluster dynamics in the LED modes. TRK sum rule is identical to the E1 sum rule when the interaction commutes with the E1 operator
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