Abstract
We investigate geometric configurations of \(\alpha \) (\(^4\)He nucleus) clusters in the second \(J^\pi =2^+\) state of \(^{12}\)C, which has been discussed as a rotational band member of the second \(0^+\) state, the Hoyle state. The ground and excited \(0^+\) and \(2^+\) states are described by a three-\(\alpha \) cluster model. The three-body Schrödinger equation with orthogonality conditions is accurately solved by the stochastic variational method with correlated Gaussian basis functions. To analyse the structure of these resonant states in a convenient form, we introduce a confining potential. The two-body density distributions together with the spectroscopic information clarify the structure of these states. We find that main configurations of both the second \(0^+\) and \(2^+\) states are acute-angled triangle shapes originating from the \(^8\)Be(\(0^+\))\(+\alpha \) configuration. However, the \(^{8}\textrm{Be}+\alpha \) components in the second \(2^+\) state become approximately 2/3 because the \(^8\)Be subsystem is hard to excite, indicating that the state is not an ideal rigid rotational band member of the Hoyle state.
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This manuscript has no associated data or the data will not be deposited. [Authors’ comment: They are available from the authors (H. Moriya or W. Horiuchi) upon reasonable request.]
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Acknowledgements
This work was in part supported by JSPS KAKENHI Grants nos. 18K03635 and 22H01214. We acknowledge the Collaborative Research Program 2022, Information Initiative Center, Hokkaido University.
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Communicated by Emiko Hiyama.
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Moriya, H., Horiuchi, W., Casal, J. et al. Three-\(\alpha \) configurations of the second \(J^\pi =2^+\) state in \(^{12}\)C. Eur. Phys. J. A 59, 37 (2023). https://doi.org/10.1140/epja/s10050-023-00947-3
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DOI: https://doi.org/10.1140/epja/s10050-023-00947-3