Fine-tuning the polymerization conditions, in particular,
solvent
medium, catalytic system, and thermodynamic parameters, it is feasible
to crystallize the growing polymer chain directly into single crystals.
Using these basic concepts, the resultant polymer, having a trans-isomer of ∼99% and a molecular weight of ∼500
kg/mol, during polymerization forms platelet-like single crystals
having crystal thickness of 7.8 nm. The crystal thickness corresponds
to the attachment of approximately 63 covalently linked carbon atoms
along the c-axis of the unit cell. Considering the
crystal thickness and chain length of approximately 37 000
covalently linked carbon atoms, electron diffraction of the nascent
crystals suggests chain folding along the ab-plane
of the single crystal. In view of the polymerization kinetics, followed
by crystallization leading to chain packing, these platelet-like single
crystals are expected to have the low entangled state. DSC thermogram
of the crystals suggests solid–solid transition from the low
entropy (monoclinic) to high entropy (hexagonal) phase, prior to melting.
The phase transition temperature, from the monoclinic to hexagonal
phase, shifts to higher temperatures on annealing crystals in the
high entropy phase. Cause for the shift in the phase transition temperature,
on annealing, is attributed to increase in crystal thickness. To follow
chain mobility during thickening, 13C solid-state NMR techniques
are employed. Similar to the trans-1,4-polybutadiene,
prepared from solution crystallization, the reversal phase transition
from the hexagonal to monoclinic phase is followed in the single crystals
by 13C solid-state NMR. The SEM images and 13C CP/MAS spectra of the nascent and the annealed single crystals
in the hexagonal phase have proven the lamellae thickening of the
isolated single crystals, accompanied by the reversal in the phase
transition to the monoclinic phase with crystal thickening. We attribute
crystal thickening in the isolated single crystals as the primary
thickening that requires high-chain mobility facilitated by the high
entropy hexagonal phase and driven by the thermodynamics of reducing
the surface energy. Amazing aspect is that the primary thickening
that requires desired cooperative motion of the covalently linked
carbon atoms reduces the crystal planar surface area to accommodate
crystal thickening that starts from several nanometers and reaches
several tens of nanometers with the phase transformation from the
monoclinic to hexagonal phase. The ease in crystal thickening, in
the high entropy phase, is suggestive of adjacent re-entry perceived
with deposition of the growing chain after suppression of the nucleation
barrier.