Chain Trajectory and Crystallization Mechanism of
a Semicrystalline Polymer in Melt- and Solution-Grown Crystals As
Studied Using <sup>13</sup>C–<sup>13</sup>C Double-Quantum
NMR
The re-entrance sites, successive
chain-folding number ⟨<i>n</i>⟩, and chain-folding
fraction ⟨<i>F</i>⟩ of the chain-folding (CF)
structure of <sup>13</sup>C CH<sub>3</sub>-labeled <i>isotactic</i> poly(1-butene) (<i>i</i>PB1) with an weight-averaged molecular
weight (⟨<i>M</i><sub>w</sub>⟩ = 37 K g/mol)
in solution- and melt-grown
crystals as a function of crystallization temperature (<i>T</i><sub>c</sub>) were determined using solid-state (SS) NMR. The solution-
and melt-grown crystals possessed adjacent re-entry structures between
the right- and left-handed stems along the (100) and (010) planes,
which were invariant as a function of <i>T</i><sub>c</sub>. The adjacent re-entry structures in the former exhibited long-range
order (⟨<i>n</i>⟩ ≥ 8) compared with
that in the latter (⟨<i>n</i>⟩ ≥ 1.7–2).
These results indicated that the concentration and entanglement of
polymers play significant roles in the CF process and structural formation
during the initial stage of crystallization, whereas kinetics does
not. Transmission electron microscopy (TEM) revealed well-defined
hexagonal and circular crystals grown from the solution state at <i>T</i><sub>c</sub> = 60 and ∼0 °C, respectively.
The morphological and molecular-level structural data demonstrated
that kinetics influences the structural formations of polymers differently
at different length scales during crystallization. Moreover, SS-NMR,
small-angle X-ray scattering (SAXS), and atomic force microscopy (AFM)
indicated that the crystallinity (χ<sub>c</sub>) and lamellar
thickness (⟨<i>l</i><sub>c</sub>⟩) of the
melt-grown crystals are highly dependent on <i>T</i><sub>c</sub>, whereas in the solution-grown crystals, these parameters
are independent of <i>T</i><sub>c</sub>. The experimental
results and molecular dynamics, as reported in the literature, indicated
that both χ<sub>c</sub> and ⟨<i>l</i><sub>c</sub>⟩ are primarily determined by the molecular dynamics of the
stems after deposition of the chains on the growth front (late process)