Abstract
The theory of nuclear beta decay induced by intense electromagnetic fields as previously presented is applied to a much broader range of physical variables. The most important intensity domain is found to occur at lower values than had previously been estimated. Furthermore, electromagnetic field ''retardation terms,'' previously pointed out as potentially important but unevaluated, are found to be significant contributors to the overall transition probability. A treatment of the entire problem in ''electric-field'' gauge, instead of the original Coulomb gauge, gives identical results.
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