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An investigation of heavy and super-heavy nuclei requires a proper model to reproduce masses and rotational energies. We had obtained in the past [1] a very good agreement with experimental data for heavy nuclei using the Yukawa folded (YF) single-particle potential [2] and the Lublin–Strasbourg Drop (LSD) [3]. The Strutinsky shell-correction method [4] and the BCS theory [5] were used to evaluate the shell and pairing energy. The equilibrium deformations of the nuclei were determined with the Modified Funny Hills (MFH) [1] shape parametrisation, and the energies of the rotational states obtained using the cranking model [6]. It was shown in Ref. [7] that a good agreement with the experimental data, especially for larger angular momenta, can only be achieved when a coupling of rotation and the pairing mode is taken into account. We are now going to extend our calculations to rotational states of super-heavy nuclei using a new Fourier-type shape

Rotational Bands in Super-heavy Nuclei Within the LSD+YF Model