Abstract
Having a detailed theoretical knowledge of the low-energy structure of the heavy odd-mass nucleus \(^{197}\hbox {Au}\) is of prime interest as the structure of this isotope represents an important input to theoretical simulations of collider experiments involving gold ions performed at relativistic energies. In the present article, therefore, we report on new results on the structure of \(^{197}\hbox {Au}\) obtained from state-of-the-art multi-reference energy density functional (MR-EDF) calculations. Our MR-EDF calculations were realized using the Skyrme-type pseudo-potential SLyMR1, and include beyond mean-field correlations through the mixing, in the spirit of the Generator Coordinate Method (GCM), of particle-number and angular-momentum projected triaxially deformed Bogoliubov quasi-particle states. Comparison with experimental data shows that the model gives a reasonable description of \(^{197}\hbox {Au}\) with in particular a good agreement for most of the spectroscopic properties of the \(3/2_1^+\) ground state. From the collective wave function of the correlated state, we compute an average deformation \(\bar{\beta }(3/2_1^+)=0.13\) and \(\bar{\gamma }(3/2_1^+)=40^\circ \) for the ground state. We use this result to construct an intrinsic shape of \(^{197}\hbox {Au}\) representing a microscopically-motivated input for precision simulations of the associated collider processes. We discuss, in particular, how the triaxiality of this nucleus is expected to impact \(^{197}\hbox {Au}\)+\(^{197}\hbox {Au}\) collision experiments at ultrarelativistic energy.
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Data availability
This manuscript has no associated data or the data will not be deposited [Authors’ comment: There is no open data associated with this article. Data from the theoretical calculations is available upon request to the authors.]
Notes
When considering axial deformations, this corresponds to a step of \(\varDelta \beta \approx 0.05\).
Note that all the extrema discussed in this article are computed from an interpolation based on the results obtained at the points on the discretized deformation mesh.
We mention in passing that some authors argue that using a \(^{198}\)Hg core provides a better global description of experimental data [6].
Provided that we interpret the \(3/2_2^+\) and \(3/2_3^+\) states as being inverted in our calculations compared to experimental data.
The trial one-quasi-particle state is built by blocking a single-particle state originating from the spherical \(2\text {d}_{3/2}\) shell.
All other non-vanishing multipole moments authorized by the symmetries of our calculations are let free to adopt a value that minimizes the total energy of the trial quasi-particle state.
We safely neglect the effect of the very small hexadecapolarity of the nucleus, \(\beta _4^{\textrm{WS}}=-0.023\), in these simulations.
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Acknowledgements
We thank Chunjian Zhang for help with the entropy-to-multiplicity conversion used in Fig. 6, and Wouter Ryssens for useful discussions. This project has received funding from the European Union’s Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement No. 839847. M.B. acknowledges support by the Agence Nationale de la Recherche, France, under grant No. 19-CE31-0015-01 (NEWFUN). G.G. is funded by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany’s Excellence Strategy EXC2181/1-390900948 (the Heidelberg STRUCTURES Excellence Cluster), within the Collaborative Research Center SFB1225 (ISOQUANT, Project-ID 273811115). The calculations were performed by using HPC resources from CIEMAT (Turgalium), Spain (FI-2021-3-0004, FI-2022-1-0004).
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Communicated by Thomas DUGUET.
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Bally, B., Giacalone, G. & Bender, M. The shape of gold. Eur. Phys. J. A 59, 58 (2023). https://doi.org/10.1140/epja/s10050-023-00955-3
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DOI: https://doi.org/10.1140/epja/s10050-023-00955-3