The $\ensuremath{\gamma}$-ray spectrum from neutron capture in the 9.47-eV resonance in $^{129}\mathrm{Xe}$ has been studied. A target of ${\mathrm{Na}}_{4}$Xe${\mathrm{O}}_{6}$ was irradiated in a thermal neutron beam and in a monochromatic neutron beam of 5.16-, 9.47-, and 14.1-eV energy from a crystal diffraction neutron monochromator. The resulting $\ensuremath{\gamma}$-ray spectra were studied with Ge(Li) detectors of $\ensuremath{\simeq}20$-, $\ensuremath{\simeq}25$-, $\ensuremath{\simeq}30$-, and $\ensuremath{\simeq}40$-${\mathrm{cm}}^{3}$ active volume. $\ensuremath{\gamma}$ rays were assigned to the $^{129}\mathrm{Xe}(n \ensuremath{\gamma})^{130}\mathrm{Xe}$ reaction by a comparison of these spectra. Ge(Li)-Ge(Li) coincidence measurements were carried out on resonance with the 20- and 30-${\mathrm{cm}}^{3}$ Ge(Li) detectors in combination. Only a few very intense transitions were observed in coincidence. The data obtained in the present work together with the information from earlier radioactive-decay studies indicate the population of levels in $^{130}\mathrm{Xe}$ by neutron capture in the 9.47-eV resonance with energies 536.1 \ifmmode\pm\else\textpm\fi{} 0.2, 1122.1 \ifmmode\pm\else\textpm\fi{} 0.3, 1204.4 \ifmmode\pm\else\textpm\fi{} 0.5, 1631.8 \ifmmode\pm\else\textpm\fi{} 0.7, 1785.9 \ifmmode\pm\else\textpm\fi{} 0.8, 1792.1 \ifmmode\pm\else\textpm\fi{} 0.6, 1807.9 \ifmmode\pm\else\textpm\fi{} 0.4, 2017.0 \ifmmode\pm\else\textpm\fi{} 0.5, 2058.7 \ifmmode\pm\else\textpm\fi{} 0.9, 2081.4 \ifmmode\pm\else\textpm\fi{} 0.9, 2171.0 \ifmmode\pm\else\textpm\fi{} 1.3, 2222.6 \ifmmode\pm\else\textpm\fi{} 0.6, 2241.5 \ifmmode\pm\else\textpm\fi{} 0.6, 2385.1 \ifmmode\pm\else\textpm\fi{} 0.5, 2501.9 \ifmmode\pm\else\textpm\fi{} 0.5, 2544.4 \ifmmode\pm\else\textpm\fi{} 0.9, 2632.4 \ifmmode\pm\else\textpm\fi{} 1.7, (2762.7 \ifmmode\pm\else\textpm\fi{} 0.5), 2885.6 \ifmmode\pm\else\textpm\fi{} 1.1, 2953.5 \ifmmode\pm\else\textpm\fi{} 0.5, 2977.5 \ifmmode\pm\else\textpm\fi{} 1.0, 3071.1 \ifmmode\pm\else\textpm\fi{} 0.8, 3150.1 \ifmmode\pm\else\textpm\fi{} 0.7, 3188.8 \ifmmode\pm\else\textpm\fi{} 0.6, (3243.2 \ifmmode\pm\else\textpm\fi{} 1.3), 3298.0 \ifmmode\pm\else\textpm\fi{} 1.2, 3325.1 \ifmmode\pm\else\textpm\fi{} 0.8, 3405.2 \ifmmode\pm\else\textpm\fi{} 0.7, 3534.2 \ifmmode\pm\else\textpm\fi{} 0.6, 3621.9 \ifmmode\pm\else\textpm\fi{} 0.7, 3685.6 \ifmmode\pm\else\textpm\fi{} 1.0, 3780.0 \ifmmode\pm\else\textpm\fi{} 1.2, 3892.2 \ifmmode\pm\else\textpm\fi{} 1.5, (3960.1 \ifmmode\pm\else\textpm\fi{} 1.0), 3976.3 \ifmmode\pm\else\textpm\fi{} 1.5, and 3985.6 \ifmmode\pm\else\textpm\fi{} 1.0 keV. The neutron separation energy of $^{130}\mathrm{Xe}$ is 9254.7 \ifmmode\pm\else\textpm\fi{} 1.3 keV. The observation of the 9254.2 \ifmmode\pm\else\textpm\fi{} 2.1 keV primary-capture $\ensuremath{\gamma}$ ray to the 0+ ground state of $^{130}\mathrm{Xe}$ clearly establishes the spin of the 9.47-eV resonance in $^{129}\mathrm{Xe}$ as 1+.[NUCLEAR REACTIONS $^{129}\mathrm{Xe}(n,\ensuremath{\gamma})$, $E=9.47$ eV; measured ${E}_{\ensuremath{\gamma}}$, ${I}_{\ensuremath{\gamma}}$, $\ensuremath{\gamma}\ensuremath{-}\ensuremath{\gamma}$ coin. in $^{130}\mathrm{Xe}$. $^{130}\mathrm{Xe}$ deduced levels, transitions, $Q$, $J$, $\ensuremath{\pi}$.]