The energies and wave functions of nonrotational states in Dy-160 that
lie below 2.3 MeV are calculated in the quasiparticle-phonon nuclear
model. Reasonably good agreement with available experimental data is o
btained, and certain predictions are made. The wave function of each o
f these excited state is dominated by a one-phonon term, the contribut
ion of a two-phonon component being below 10%. It is shown that the fr
agmentation of one-phonon states with energies above 2.5 MeV is signif
icant and must therefore be taken into account. The quantities B(E1) a
nd B(M1) for transitions from the ground state to excited states below
4 MeV are calculated with allowance for the fragmentation of one-phon
on states. The results are found to be in qualitative agreement with e
xperimental data. The orbital and spin parts of the M1 operator make c
lose contributions to B(M1) values for the excitation of If states wit
h energies in the range 2.3 - 3.3 MeV. It is demonstrated that the enh
anced E1, E2, and M1 transitions furnish information about two-phonon
components of the wave functions of excited states.