Abstract
The concept of intermediate structure or doorway states [23] has been most useful in the understanding of a wide range of phenomena in nuclear reactions including isobaric analogue resonances, the giant dipole resonance and neutron induced fission. In each of these examples, the primary characteristic of the doorway state is a relatively simple structure which is easily excited in the entrance channel. The strength of the coupling of this state to the many model of decay which may be energetically allowed determines its width and the ease with which it may be observed experimentally.
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