Ethylene/1-octene
statistical multiblock copolymers (OMBCs) consisting
of the alternation of crystalline, hard blocks and amorphous, soft
blocks, with ≈0.5 and 20 mol % of 1-octene units, respectively,
are subjected to thermal fractionation resorting to successive self-nucleation
and annealing (SSA). The study is extended to random copolymers (RCs)
of high (44 kDa) and low (3.4 kDa) number average molecular mass M
n, mimicking in 1-octene content the crystalline
hard blocks and to the OMBC fractions extracted in boiling n-hexane and cyclohexane through a suitable solution fractionation
protocol. For all the samples, the melting endotherms are well resolved
in a multiplicity of peaks corresponding to the melting of crystals
of different thicknesses generated in the SSA protocol that reflect
the distribution of the methylene sequence length (MSL) in between
consecutive interruptions along the chains. It is shown that, regardless
of molecular mass, the MSL distributions of the RC samples are shifted
toward greater values than those of the OMBC samples, and that also
the shapes of the distributions are different. Since the MSL distribution
depends on the frequency and distribution of the defects along the
chains, and the defects act as interruption points, the higher fraction
of long crystallizable sequences in the RC samples suggests that whereas
for the RC samples the interruptions are merely represented by the
1-octene units that are rejected outside the crystals, for the OMBCs,
the interruption of the regular methylene sequences belonging to the
crystalline hard blocks due to the amorphous soft blocks linked to
them should also play a role. Indeed, due to the partial miscibility
of the hard and soft blocks, the hard blocks of major length tend
to crystallize in a confined environment. This prevents the formation
of thicker crystals and induces decrease of the MSL values as well
as changes in the shape of the MSL distributions (topological confinement).
On the other hand, the hard blocks of shorter length tend to crystallize,
crossing the hard block rich regions and causing melting point depression
and consequent shift of the MSLs toward lower values with respect
to RCs (diluent effect). It is shown that differences in the MSL distribution
of OMBCs are the result of the interplay between topological confinement
and diluent effect, which in turn reflects differences in the OMBC
chain microstructure, that is, differences in the distribution of
block length at the inter- and intra-chain level.