We report on theoretical total cross sections for electron capture from the ground state of atomic hydrogen $\mathrm{H}\left(1s\right)$ by fast multiply-charged nuclei ${\mathrm{H}}^{+},$ ${\mathrm{He}}^{2+},$ ${\mathrm{Li}}^{3+},$ ${\mathrm{Be}}^{4+},$ ${\mathrm{B}}^{5+},$ ${\mathrm{C}}^{6+},$ ${\mathrm{N}}^{7+},$ ${\mathrm{O}}^{8+}$ and ${\mathrm{F}}^{9+}.$ The prior form of the boundary-corrected continuum intermediate states (BCIS) method is used. For a single fixed initial ground-state $(i=1s),$ comprehensive computations are carried out for a sequence of the transitions to the final state $(n,l,m)$ with $1\le n\le n_{max},$ including all the energy degenerate sub-levels $(-l\le m\le l,0\le l\le n-1).$ The maximal quantum number $n_{max}$ is respectively set to 4 for ${\mathrm{H}}^{+},$ ${\mathrm{He}}^{2+}$ and ${\mathrm{Li}}^{3+},$ to 5 for ${\mathrm{Be}}^{4+},$ to 6 for ${\mathrm{B}}^{5+},$ as well as to 7 for ${\mathrm{C}}^{6+},$ ${\mathrm{N}}^{7+},$ ${\mathrm{O}}^{8+}$ and ${\mathrm{F}}^{9+}.$ The reported nine tables provide these state-selective cross sections ($Q_{if}$) and their state-summed counterparts ($Q_{\Sigma }$). The cross sections $Q_{\Sigma }$ for the sum over all the final states are evaluated using the exact results of $Q_{if}$ for $n\le n_{max}$ and the scaled cross sections for $n>n_{max}.$ The scaling is based on the Oppenheimer $n^{-3}$ rule. In addition to these tables, at the same impact energies 20–3000 keV/amu, the cross sections from the BCIS method are presented graphically in eight figures for the nuclei ${\mathrm{Li}}^{3+},{\mathrm{Be}}^{4+},{\mathrm{B}}^{5+},{\mathrm{C}}^{6+},{\mathrm{N}}^{7+},{\mathrm{O}}^{8+}$ and ${\mathrm{F}}^{9+}.$ This complements our recently published cross sections for electron capture by protons (${\mathrm{H}}^{+}$) and alpha particles (${\mathrm{He}}^{2+}$) from $\mathrm{H}\left(1s\right).$ In the present figures, whenever available, the corresponding experimental data are compared with our results for $Q_{\Sigma }.$ Also included in these comparisons are the corresponding results for $Q_{\Sigma }$ from the continuum distorted wave (CDW) method. The cross sections tabulated here can be used in versatile applications ranging from plasma physics and astrophysics through fusion research to ion therapy.

我们报告了从氢原子基态捕获电子的理论总截面 $\mathrm{H}（\mathrm{1个}s）$ 通过快速倍增核 ${\mathrm{H}}^{+}，$ ${\mathrm{他}}^{\mathrm{2个}+}，$ ${\mathrm{里}}^{3+}，$ ${\mathrm{是}}^{4+}，$ ${\mathrm{乙}}^{5+}，$ ${\mathrm{C}}^{6+}，$ ${\mathrm{ñ}}^{7+}，$ ${\mathrm{Ø}}^{8+}$ 和 ${\mathrm{F}}^{9+}。$使用边界校正的连续统中间态（BCIS）方法的先验形式。对于单个固定的初始基态$（\mathrm{一世}=\mathrm{1个}s），$ 对过渡到最终状态的序列进行了全面的计算 $（ñ，升，米）$ 和 $\mathrm{1个}\le ñ\le {ñ}_{最大限度}，$ 包括所有能量退化子级别 $（-升\le 米\le 升，0\le 升\le ñ-\mathrm{1个}）。$ 最大量子数 ${ñ}_{最大限度}$ 分别设置为4 ${\mathrm{H}}^{+}，$ ${\mathrm{他}}^{\mathrm{2个}+}$ 和 ${\mathrm{里}}^{3+}，$ 到5 ${\mathrm{是}}^{4+}，$ 到6 ${\mathrm{乙}}^{5+}，$ 以及7 ${\mathrm{C}}^{6+}，$ ${\mathrm{ñ}}^{7+}，$ ${\mathrm{Ø}}^{8+}$ 和 ${\mathrm{F}}^{9+}。$ 报告的9个表格提供了这些状态选择的横截面（${问}_{\mathrm{一世}F}$）和其状态求和的对应项（${问}_{\Sigma }$）。横截面${问}_{\Sigma }$ 对于所有最终状态的总和，将使用的精确结果进行评估 ${问}_{\mathrm{一世}F}$ 为了 $ñ\le {ñ}_{最大限度}$ 和比例横截面 $ñ>{ñ}_{最大限度}。$ 缩放比例基于Oppenheimer ${ñ}^{-3}$规则。除了这些表格以外，在相同的冲击能量20–3000 keV / amu时，BCIS方法的横截面以图形形式以八位图形显示在原子核上${\mathrm{里}}^{3+}，{\mathrm{是}}^{4+}，{\mathrm{乙}}^{5+}，{\mathrm{C}}^{6+}，{\mathrm{ñ}}^{7+}，{\mathrm{Ø}}^{8+}$ 和 ${\mathrm{F}}^{9+}。$ 这补充了我们最近发布的质子捕获电子的截面（${\mathrm{H}}^{+}$）和alpha粒子（${\mathrm{他}}^{\mathrm{2个}+}$） 从 $\mathrm{H}（\mathrm{1个}s）。$ 在本图中，只要有可用的数据，就会将相应的实验数据与我们的结果进行比较 ${问}_{\Sigma }。$ 这些比较中还包括 ${问}_{\Sigma }$从连续畸变波（CDW）方法中得出。此处列出的横截面可用于多种应用，从等离子物理学和天体物理学到聚变研究再到离子治疗。