  The scissors mode is investigated in the actinides region, including
even-even superheavy nuclei up to $^{256}$No, within the Time Dependent
Hartree-Fock-Bogoliubov (TDHFB) approach. The solution of TDHFB equations by
the Wigner Function Moments (WFM) method predicts a splitting of the scissors
mode into three intermingled branches due to spin degrees of freedom. Both the
calculated energy centroid and integrated $M1$ strength in $^{254}$No are in
good agreement with the results of recent measurements performed by the Oslo
method. The energy centroids and summed $B(M1)$ values for others transuranium
nuclides are predicted. The calculations are performed also for $^{232}$Th and
$^{236,238}$U isotopes using an updated compilation of deformation parameters.
The results are compared with that obtained previously by WFM theory and with
the latest experimental data. Progress has been achieved in theoretical
understanding of the origins of double-humped structure of scissors spectrum
observed in the Actinides.
