Three- configurations of the second state in C
arXiv:2302.02539 · doi:10.1140/epja/s10050-023-00947-3
Abstract
We investigate geometric configurations of (He nucleus) clusters in the second state of C, which has been discussed as a rotational band member of the second state, the Hoyle state. The ground and excited and states are described by a three- 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 and states are acute-angled triangle shapes originating from the Be() configuration. However, the Be components in the second state become approximately 2/3 because the 8Be subsystem is hard to excite, indicating that the state is not an ideal rigid rotational band member of the Hoyle state.
arXiv comment7 pages, 3 figures
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