Abstract
In a phenomenological approach, the \(\alpha \) + core structure is investigated in the \(^{20}\)Ne, \(^{44}\)Ti, \(^{94}\)Mo, \(^{104}\)Te, and \(^{212}\)Po nuclei through the local potential model using a double-folding nuclear potential with effective nucleon-nucleon interaction of M3Y + \(c_{\textrm{sat}}\delta (s)\) type, where the term \(c_{\textrm{sat}}\delta (s)\) acts only between the saturation regions of \(\alpha \)-cluster and core. Properties such as energy levels, \(\alpha \)-widths, B(E2) transition rates, and half-lives are calculated, and good level of agreement with experimental data is obtained in general. It is shown the inclusion of the term \(c_{\textrm{sat}}\delta (s)\) is determinant for a better description of the experimental energy levels compared to the ground state bands produced with the simple M3Y interaction. The properties calculated for \(^{104}\)Te reinforce the superallowed \(\alpha \)-decay feature for this nucleus, as indicated in previous studies.
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This manuscript has no associated data or the data will not be deposited. [Authors’ comment: As a theoretical physics publication, there is no experimental data to be shared.]
Notes
Details on the values of \(\lambda \), \(c_{\textrm{sat}}\), and R adopted for \(^{104}\)Te are discussed in Sect. 3.
The \(^{94}\)Mo experimental negative parity band presents levels from (5)\(^{-}\) (\(E_x = 2.611\) MeV) to (\(17^{-}\)) (\(E_x = 7.782\) MeV) connected by \(\gamma \)-transitions [33]; however, the excited state (5)\(^{-}\) undergoes a \(\gamma \)-transition to the \(4^{+}\) state (\(E_x = 1.574\) MeV) of the \(G = 16\) g.s. band. As the excited state (5)\(^{-}\) does not undergo a transition of \(J \rightarrow J - 2\) type, the \(G = 17\) band is assumed to be incomplete and the calculation of the corresponding theoretical band is made from \(J^{\pi } = 5^{-}\).
The recent experimental works of von Tresckow et al. [2] and Karayonchev et al. [46] present the measures \(B(E2;6^{+}_{1} \rightarrow 4^{+}_{1}) = 8.7(15)\) W.u. and \(9.0(+9 \; -7)\) W.u. for \(^{212}\)Po, respectively, which favors the theoretical predictions of Refs. [7, 9, 12]. However, the 2020 \(^{212}\)Po experimental data compilation [34, 50] presents the value \(B(E2;6^{+}_{1} \rightarrow 4^{+}_{1}) = 13.2(+49 \; -29)\) W.u. shown in Table 6.
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The authors thank the HPC resources provided by Information Technology Superintendence (HPC-STI) of University of São Paulo. Support from Instituto Nacional de Ciência e Tecnologia – Física Nuclear e Aplicações (INCT-FNA) is acknowledged.
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Souza, M.A., Miyake, H. \(\alpha \) + core structure described with an additional interaction in the nuclear matter saturation region. Eur. Phys. J. A 59, 74 (2023). https://doi.org/10.1140/epja/s10050-023-00990-0
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DOI: https://doi.org/10.1140/epja/s10050-023-00990-0