The (excess) power spectrum J
Γ
of the depolarized component of scattered light intensity
was measured for eight samples of isotactic oligo- and poly(methyl
methacrylate)s (i-PMMA), each with
the fraction of racemic diads f
r ≃ 0.01, in
the range of weight-average degree of polymerization
x
w from
4 to 70.1 in acetonitrile at 28.0 °C (ϑ). The spin−lattice
relaxation time T
1 was also determined for
the
three samples with x
w = 4, 5, and 70.1, and
the nuclear Overhauser enhancement NOE, for the two
samples with x
w = 4 and 70.1, all in
acetonitrile at 35 °C. As in the cases of atactic (a-)
polystyrene
(a-PS) and a-PMMA previously studied, it is found that
J
Γ may be well represented in terms of a
single
Lorentzian independently of x
w and that the
relaxation time τΓ defined from
J
Γ at infinite dilution increases
with increasing x
w and levels off to its
asymptotic value in the limit of x
w → ∞,
being consistent with the
recent theoretical prediction on the basis of the helical wormlike (HW)
chain model. A comparison is
made of the present data for τΓ,
T
1, and NOE with the HW theory, and it is shown
that the theory may
explain satisfactorily the data in the range of
x
w ≳ 10, although semiquantitatively for
τΓ. For x
w ≲
10,
the rigid sphere model having the radius equal to the apparent
root-mean-square radius of gyration of
the HW chain may give a good explanation of τΓ but not
of T
1, indicating that the dynamic
depolarized
light scattering and nuclear magnetic relaxation cannot be described in
terms of a common single
relaxation time. However, there is shown to be an effective (mean)
magnetic relaxation time τM
approximately equal to 0.6τΓ. From a comparison of
the present results for τΓ for i-PMMA with the
previous
ones for a-PS and a-PMMA, it is shown that there is good correlation
between the static and dynamic
chain stiffness, the latter being defined as the ratio of the value of
τΓ in the limit of x
w → ∞ to
that of the
corresponding isolated repeat unit (monomer), as predicted by the HW
theory.