The equilibrium properties and the Rouse-Zimm dynamics of polymer mole
cules with any architecture at temperatures T less than or equal to Th
eta, are treated using a bead-and-spring coarse-grained description. T
he collapsed globule model is adopted, whereby essentially all atoms a
re at the same mean-square distance (S-2) from the center of mass; acc
ordingly, at a given temperature the interatomic free energy is a sing
le-valued function of (S-2) and the self-consistent free-energy minimi
zation is greatly simplified, in the Gaussian approximation. We prove
that the connectivity matrix B and the bond-vector product matrix M=[(
I-i.I-j)] possess the same eigenvectors; these are the normal modes of
the chain conformation. Furthermore, we show that (S-2)=N(at)(-1)Sigm
a(k)l(2) alpha(k)(2)/lambda(k), where N-at is the total number of atom
s, lambda(k) is the general nonzero eigenvalue of B, and l(2) alpha(k)
(2) is the corresponding eigenvalue of M-the expansion ratio of the no
rmal mode. Finally, we prove that in the free-draining limit the norma
l mode relaxation times are proportional to l(2) alpha(k)(2)/lambda(k)
. Defining as alpha(s)=root(S-2)/(S-2)(ph) as the overall strain ratio
with respect to the phantom state, the plots of alpha(s) vs the reduc
ed temperature tau=(T-Theta)/T less than or equal to 0 indicate that p
olymers with more compact architectures display a prompter contraction
for small \tau\'s, although tending to larger alpha(s)'s at strong un
dercoolings, where the average density (alpha N-at.(S-2)(-3/2)) is abo
ut the same for all architectures. Concerning the dynamical behavior,
at sufficiently large \tau\'s the longest relaxation times reach a typ
ical plateau, as already found for the linear chain.