In this work we report on ab initio theoretical results for the magnetic-field-induced 2s 2p 3 P 0 → 2s 2 1 S 0 E1 transition for ions in the beryllium isoelectronic sequence between Z = 5 and 92. It has been proposed that the rate of the E1M1 two-photon transition 2s 2p 3 P 0 → 2s 2 1 S 0 can be extracted from the lifetime of the 3 P 0 state in Be-like ions with zero nuclear spin by employing resonant recombination in a storage ring. This experimental approach involves a perturbing external magnetic field. The effect of this field needs to be evaluated in order to properly extract the two-photon rate from the measured decay curves. The magnetic-field-induced transition rates are carefully evaluated, and it is shown that, with a typical storage-ring field strength, it is dominant or of the same order as the E1M1 rate for low-and mid-Z ions. Results for several field strengths and ions are presented, and we also give a simple Z-dependent formula for the rate. We estimate the uncertainties of our model to be within 5% for low-and mid-Z ions and slightly larger for more highly charged ions. Furthermore we evaluate the importance of including both perturber states, 3 P 1 and 1 P 1 , and it is shown that excluding the influence of the 1 P 1 perturber overestimates the rate by up to 26% for the mid-Z ions.