The three-body boundary-corrected continuum intermediate state (BCIS-3B) method is employed to compute single-electron capture cross sections. These data are for collisions in which a target helium atom in its ground state $\mathrm{He}\left(1s^2\right)$ is impacted by multiply charged nuclei (specifically ${\mathrm{H}}^{+},{\mathrm{He}}^{2+},{\mathrm{Li}}^{3+},{\mathrm{Be}}^{4+},{\mathrm{B}}^{5+},{\mathrm{C}}^{6+},{\mathrm{N}}^{7+},{\mathrm{O}}^{8+},{\mathrm{F}}^{9+}$). Intermediate and high projectile energies are considered (20 keV/amu-3 MeV/amu). The obtained results are tabulated for total cross sections (state-selective $Q_{nlm}$ as well as state-summed $Q_{nl},$ $Q_n$ and $Q_{\Sigma }$). Cross section $Q_{nlm}$ corresponds to a fixed triple of the hydrogenlike quantum numbers $\{n,l,m\}.$ In $Q_{nl},Q_n$ and $Q_{\Sigma },$ the sums over $m\in [-l,l],l\in [0,n-1]$ and $n\in [1,n_{\max }]$ are carried out, respectively. For $n>n_{\max }$ in $Q_{\Sigma },$ the Oppenheimer $n^{-3}$ scaling rule is adopted. The values of $n_{\max }$ are set to 4 (for ${\mathrm{H}}^{+},{\mathrm{He}}^{2+},{\mathrm{Li}}^{3+}$), 5 (for ${\mathrm{Be}}^{4+}$), 6 (for ${\mathrm{B}}^{5+}$) and 7 (for ${\mathrm{C}}^{6+},{\mathrm{N}}^{7+},{\mathrm{O}}^{8+},{\mathrm{F}}^{9+}$). Exhaustive comparisons of the theoretical findings for $Q_{\Sigma }$ with the corresponding experimental data are performed. It is determined that the BCIS-3B method is in excellent agreement with the available measurements. The present database for the examined capture processes is deemed to be of notable practical usefulness in versatile applications of particular relevance to plasma physics, astrophysics, fusion research and ion therapy in medicine.

采用三体边界校正连续介质中间态 (BCIS-3B) 方法计算单电子捕获截面。这些数据用于碰撞，其中目标氦原子处于基态$\mathrm{他}\left(1s^2\right)$受到多电荷核的影响（特别是${\mathrm{H}}^{+},{\mathrm{他}}^{2+},{\mathrm{李}}^{3+},{\mathrm{是}}^{4+},{\mathrm{乙}}^{5+},{\mathrm{C}}^{6+},{\mathrm{ñ}}^{7+},{\mathrm{○}}^{8+},{\mathrm{F}}^{9+}$）。考虑了中等和高射弹能量（20 keV/amu-3 MeV/amu）。获得的结果列在总横截面列表中（状态选择性${问}_{nl米}$以及状态总和${问}_{nl},$ ${问}_n$和${问}_{\Sigma }$）。横截面${问}_{nl米}$对应于类氢量子数的固定三元组$\{n,l,米\}.$在${问}_{nl},{问}_n$和${问}_{\Sigma },$总和$米\in [-l,l],l\in [0,n-1]$和$n\in [1,n_{\mathrm{最大限度}}]$分别进行。为了$n>n_{\mathrm{最大限度}}$在${问}_{\Sigma },$奥本海默$n^{-3}$采用缩放规则。的价值观$n_{\mathrm{最大限度}}$设置为 4 （对于${\mathrm{H}}^{+},{\mathrm{他}}^{2+},{\mathrm{李}}^{3+}$), 5 (对于${\mathrm{是}}^{4+}$), 6 (对于${\mathrm{乙}}^{5+}$) 和 7 (对于${\mathrm{C}}^{6+},{\mathrm{ñ}}^{7+},{\mathrm{○}}^{8+},{\mathrm{F}}^{9+}$）。理论结果的详尽比较${问}_{\Sigma }$进行相应的实验数据。确定 BCIS-3B 方法与可用测量值非常一致。用于检查的捕获过程的当前数据库被认为在与等离子体物理学、天体物理学、融合研究和医学离子疗法特别相关的多功能应用中具有显着的实际用途。