Abstract
It is argued here that (at least light) nuclei may reside in a sweet spot: bound weakly enough to be insensitive to the details of the interaction, but dense enough to be insensitive to the exact values of the large two-body scattering lengths as well. In this scenario a systematic expansion of nuclear observables around the unitarity limit converges. In particular, the nuclear force in this scheme is constructed such that the gross features of states in the nuclear chart are determined by a very simple leading-order interaction, whereas—much like the fine structure of atomic spectra—observables are moved to their physical values by small perturbative corrections. Explicit evidence in favor of this conjecture is shown for the binding energies of three and four nucleons.
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Acknowledgements
I would like to thank Harald Grießhammer, Hans-Werner Hammer, and Bira van Kolck for their collaboration as well as for many insightful discussions and comments on this manuscript. This work was supported in part by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) – Projektnummer 279384907 – SFB 1245 and by the ERC Grant No. 307986 STRONGINT.
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König, S. (2020). The Unitarity Expansion for Light Nuclei. In: Orr, N., Ploszajczak, M., Marqués, F., Carbonell, J. (eds) Recent Progress in Few-Body Physics. FB22 2018. Springer Proceedings in Physics, vol 238. Springer, Cham. https://doi.org/10.1007/978-3-030-32357-8_54
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