Abstract
In a broad sense, light-induced atomic states are decaying bound states that exist in sufficiently strong laser fields but cannot be adiabatically followed to zero intensity as physical quasistationary states. Some of them have no counterpart in the field-free bound-state spectrum. The paper contains a short review of the literature concerning this topic. It addresses two issues: the origin of the light-induced states in Floquet theory, and their relevance.
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