In the first part of this work, we study the quadrupole collective properti
es of N-a = 2, 4, 6, and 8 nucleons occupying the abnormal-parity intruder
single-particle states with high angular momenta j(a) = 9/2, 11/2, 13/2, an
d 15/2. This study is essential for a detailed understanding of the contrib
ution made by these nucleons to the quadrupole collectivity of the yrast st
ares of deformed nuclei. The properties studied include (i) the distributio
n of the angular momenta J contained in the intrinsic state of N-a particle
s in the \j(a)k(a)] states, (ii) the relationship between the quadrupole mo
ment Q(0)(j(a),N-a) of such an intrinsic state and the maximum angular mome
ntum J(max) contained in it, (iii) the complete set of reduced quadrupole m
atrix elements (J'parallel to Q parallel to J) for transitions between all
the states \J] and \J'] projected from the intrinsic state, (iv) the B(E2:J
-->J-2) values, (v) the transition moments Q(t)(J), and (vi) the spectrosco
pic quadrupole moment Q(J). We compare these properties with similar proper
ties of an intrinsic state having SU(3) symmetry which contains the same se
t of angular momenta as contained in the intrinsic state of a particular nu
mber of nucleons in a specific j(a) configuration. In the second part, we u
se the input from the first part to study the collective properties of the
coupled system of protons and neutrons in abnormal-parity states. We show t
hat the SU(3)-like features observed for the individual groups of abnormal-
parity nucleons become stronger for the coupled system. Finally, in the thi
rd part, we consider the yrast bands of well-deformed nuclei projected from
their Nilsson intrinsic states of valence nucleons in a major shell. We sp
ecify the structure of the wave function of each projected yrast state \J]
in terms of the nucleons in both normal- and abnormal-parity states. These
wave functions can be used to determine the individual contributions of the
nucleons in normal- and abnormal-parity states to any specific property of
the yrast state. In particular, we calculate the transition moments Q(t)(J
) of the entire yrast band of even-even Yb160-166, Dy-156,Dy-158, Th-232, U
-234, and U-236 projected from their respective Nilsson intrinsic states.