Anti-halo effects on reaction cross sections for ${}^{14,15,16}$C isotopes

Abstract

We study anti-halo effects on reaction cross sections ${\sigma }_{\mathrm{R}}$ for ${}^{14,15,16}$C scattering from a ${}^{12}$C target at 83~MeV/nucleon, using the $g$-matrix double-folding model. ${}^{15}$C is described by the ${}^{14}$C~+~$n$ two-body model that reproduces the measured large s-wave spectroscopic factor, i.e., the shell inversion that the 1s${}_{1/2}$ orbital is lower than the 0d${}_{5/2}$ orbital in energy. ${}^{16}$C is described by the ${}^{14}$C~+~$n$~+~$n$ three-body model with the phenomenological three-body force (3BF) that explains the measured small s-wave spectroscopic factor. The 3BF allows the single-particle energies of the ${}^{14}$C + $n$ subsystem to depend on the position $r$ of the second neutron from the center of mass of the subsystem. The 1s${}_{1/2}$ orbital is lower than the 0d${}_{5/2}$ orbital for large $r$, but the shell inversion is restored for small $r$. Anti-halo effects due to the "partial shell inversion" make ${\sigma }_{\mathrm{R}}$ for ${}^{16}$C smaller than that for ${}^{15}$C. We also investigate projectile breakup effects on the mass-number dependence of ${\sigma }_{\mathrm{R}}$ with the continuum discretized coupled-channels method.

arXiv comment5pages, 4 figures

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• Three-body description of ${}^9$C: Role of low-lying resonances in breakup reactions
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