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Potential roots of the deep subbarrier heavy-ion fusion hindrance phenomenon within the sudden approximation approach

Peiwei WenChina Institute of Atomic Energy, 102413 Beijing, ChinaC. J. LinChina Institute of Atomic Energy, 102413 Beijing, ChinaR. G. NazmitdinovDubna State University, 141982 Dubna, RussiaS. I. VinitskyJoint Institute for Nuclear Research, 141980 Dubna, RussiaО. ЧулуунбаатарInstitute of Mathematics and Digital Technology, Mongolian Academy of Sciences, 13330 Ulaanbaatar, MongoliaА. А. ГусевDubna State University, 141982 Dubna, RussiaA. K. NasirovInstitute of Nuclear Physics, Ulugbek, 100214 Tashkent, UzbekistanH. M. JiaChina Institute of Atomic Energy, 102413 Beijing, ChinaA. GóźdźInstitute of Physics, University of M. Curie-Skłodowska, 520031 Lublin, Poland
Physical review. Cjournal2021en
ABI

Abstract

We analyze the origin of the unexpected deep subbarrier heavy-ion fusion hindrance in $^{64}\mathrm{Ni}+^{100}\mathrm{Mo}$, $^{64}\mathrm{Ni}+^{64}\mathrm{Ni}$, and $^{28}\mathrm{Si}+^{64}\mathrm{Ni}$ reactions. Our analysis is based on the improved coupled-channels description, implemented by means of the finite element method. With the aid of the Woods-Saxon potential the experimental cross sections and the $S$ factors of these reactions are remarkably well reproduced within the sudden approximation approach. We found that accounting for the nondiagonal matrix elements of the coupling matrix, traditionally neglected in the conventional coupled-channels approaches in setting the left boundary conditions inside the potential pocket, and its minimal value are crucially important for the interpretation of experimental data. We found as well a good agreement with the general trend of the experimental data for the $S$ factor of the fusion reaction $^{12}\mathrm{C}+^{12}\mathrm{C}$, which has no pronounced maximum for this system.

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