Abstract

An approach describing the thermal damping width of the giant dipole resonance (GDR) in hot nuclei is presented. The GDR is generated by the ph excitations within the finite-temperature random-phase approximation (FTRPA), while its damping at finite temperature arises from irreversible coupling of ph configurations to the thermal pp and hh ones beyond the FTRPA. A semimicroscopic unification of the quantal spreading and thermal damping widths is undertaken within the framework of motional damping. The numerical calculations are performed, using a schematic model with equally degenerate equidistant shells for a hot nucleus of mass A=112 carrying no angular momentum. The results show that the total width of the GDR increases strongly as a function of the excitation energy up to E{sup {asterisk}}{approximately}120{endash}130 MeV, where it reaches a saturation value. The limiting temperature for the GDR in very hot nuclei is discussed. {copyright} {ital 1997} {ital The American Physical Society}

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