  The Skyrme energy-density functionals with modified spin-spin interaction and
pairing strength are used for description of the $^{249}$No, $^{251}$No, and
$^{253}$No excited states. The results of the HFB and cranked HFB calculations
taking into account the blocking effect are in reasonable agreement with the
available data. For many states, including rotational and three-quasiparticle
states, the results of self-consistent calculations were obtained for the first
time.
