In this work we study the radiative capture of on ${\rm {}^4He}$ within the halo effective field theory (EFT) framework. At leading order the capture amplitude comprises the initial state -wave strong and Coulomb interactions summed to all orders. At the same order in the expansion, leading two-body currents contribute as well. We find delicate cancelations between the various contributions, and the two-body current contributions can be replaced by appropriately enhancing the asymptotic normalizations of the Be ground and first excited state wave functions. The next-to-leading order corrections come from the -wave shape parameter and the pure Coulomb -wave initial state interactions. We fit the EFT parameters to available scattering data and most recent capture data. Our zero-energy astrophysical -factor estimate, keV b, is consistent within error bars with the average in the literature.

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