  We report a leading-order calculation of radiative ${}^{7}\mathrm{Li}$
neutron captures to both the ground and first excited state of
${}^{8}\mathrm{Li}$ in the framework of a low-energy effective field theory
(Halo-EFT). Each of the possible final states is treated as a shallow bound
state composed of both $n+{}^{7}\mathrm{Li}$ and $n+{}^{7}\mathrm{Li}^{*}$
(core excitation) configurations. The {\it ab initio} variational Monte Carlo
method is used to compute the asymptotic normalization coefficients of these
bound states, which are then used to fix couplings in our EFT. We calculate the
total and partial cross sections in the radiative capture process using this
calibrated EFT. Fair agreement with measured total cross sections is achieved
and excellent agreement with the measured branching ratio between the two final
states is found. In contrast,a previous Halo-EFT calculation [G. Rupak and R.
Higa, Phys. Rev. Lett {\bf 106}, 222501 (2011)] assumes that the
$n$-${}^{7}\mathrm{Li}$ couplings in different spin channels are equal, fits
the $P$-wave "effective-range" parameter to the threshold cross section for
${}^7{\rm Li} + n \rightarrow {}^8{\rm Li} + \gamma$, and assumes the core
excitation is at high enough energy scale that it can be integrated out.
