The quasi-SU(3) symmetry was uncovered in full pf and sdg shell-model calcu
lations for both even-even and odd-even nuclei. It manifests itself through
a dominance of single-particle and quadrupole-quadrupole terms in a Hamilt
onian used to describe well-deformed nuclei. A practical consequence of the
quasi-SU(3) symmetry is an efficient basis truncation scheme. In [C.E. Var
gas et al., Phys. Rev. C 58 (1998) 1488] it is shown that when this type of
Hamiltonian is diagonalized in an SU(3) basis, only a few irreducible repr
esentations (irreps) of SU(3) are needed to describe the yrast band, the le
ading S = 0 irrep augmented with the leading S = 1 irreps in the proton and
neutron subspaces. In the present article the quasi-SU(3) truncation schem
e is used, in conjunction with a "realistic but schematic" Hamiltonian that
includes the most important multipole terms, to describe the energy spectr
a and B(E2) transition strengths of Ne-20,Ne-22, Mg-24 and Si-28. The effec
t of the size of the Hilbert space on both sets of observables is discussed
, as well as the structure of the yrast band and the importance of the vari
ous terms in the Hamiltonian. The limitations of the model are explicitly d
iscussed. (C) 2001 Elsevier Science B.V. All rights reserved.