The fold surfaces of polymer crystals may become suitable
nucleating
sites for uncrystallized material left over during the primary crystallization
process. This “nucleation by the folds surface” (NFS)
ability is highlighted in the so-called polymer decoration technique
in which vapors of polyethylene condense and crystallize on a cold
fold surface substrate to form edge-on lamellae that reveal the folds
and loops orientations in different growth sectors. In bulk materials,
the primary crystallization leaves confined and uncrystallized material
between lamellae. NFS, based on epitaxy-type interactions, is expected
to take place in these confined and supercooled melt fractions before “true” homogeneous nucleation sets
in. The insights provided help elucidate the structural features of the interlamellar layers of crystalline polymers, which overcomes
the limits of global, indirect investigation techniques (e.g., differential
scanning calorimetry (DSC)) used in attempts to analyze their structure
in situ. The interlamellar layer is known to be divided into a rigid
amorphous fraction (RAF) located in contact with the fold surfaces
and a mobile amorphous fraction (MAF) at its center. The nature of
the RAFamorphous but rigid above its T
g, or crystallineis still debated. The NFS provides
a structural identity for the RAF that associates conformation disorder
with stem orientation: the RAF is actually a “condis oriented”
fraction. On heating, the small endotherm observed in DSC curves corresponds
to its isotropization. The RAF is also a protonucleus for secondary
crystallization and induces the growth of edge-on lamellae on top
and in the interlamellar spaces of the primary crystals. As such,
the RAF has also a layered lamellar structure. Polymer decoration,
the “condis oriented” RAF, and the specific edge-on
lamellar secondary crystallization are manifestations of the nucleation
by the fold surfaces.