A systematic analysis of rotational bands in doubly odd nuclei in the
mass region A = 130-140 is carried out using a shell model configurati
on mixing approach. The shell model (many-body) basis is constructed b
y projecting out deformed quasiparticle (Nilsson + BCS) states onto go
od angular momenta. The hamiltonian is assumed to be a sum of (spheric
al) single-particle hamiltonian and a schematic two-body interaction,
which consists of Q . Q + (monopole) pairing + quadrupole-pairing forc
es. The analysis indicates a shape transition from prolate (N = 73) to
oblate (N = 79) shape as a function of neutron number. Agreement betw
een theoretical results and experimental data is quite satisfactory ex
cept for gamma-deformed nuclei (N = 75 and 77).