Abstract
Realistic calculations of the pair transfer strength functions were performed for the nuclei /sup 162/Dy and /sup 164/Dy as a function of the angular momentum and excitation energy in the frame of the self-consistent, cranked Hartree-Fock-Bogoliubov and random-phase-approximation theories. At low angular momenta most of the strength is concentrated in the ground-to-ground transition, whereas at high angular momenta, after the pairing correlation has dropped, the strength is spread among several states located a few (less than or equal to4) MeV above the yrast line.
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