BCC Grain Formation Triggered by Miscibility Jump
on Temperature Drop
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Abstract
Formation of a body-centered cubic
(BCC) structure and grain growth
process triggered by segregation-power jump on a temperature drop
was studied by small-angle X-ray scattering (SAXS), rheology, and
differential scanning calorimetry (DSC). Polystyrene-<i>block</i>-poly(ethylene-<i>alt</i>-propylene) (SEP) was dissolved
in tridecyl-2,2,4-trimethyl hexanoate (salacos913) that was a practically
neutral good solvent for both of polystyrene (PS) and PEP block chains
at temperature above 84 °C (<i>T</i><sub>sol</sub>),
while it was highly selective (good for PEP) below <i>T</i><sub>sol</sub>. Spherical microdomains in a short-range liquid-like
order were formed above <i>T</i><sub>sol</sub>; the system
was in the so-called “lattice disordered state”, designated
as disordered sphere. The solution was annealed at a temperature (130
°C) above <i>T</i><sub>sol</sub> for 10 min and successively
subjected to a temperature drop across <i>T</i><sub>sol</sub>. The system stayed in the lattice-disordered state for a certain
induction period. During this induction period, stronger segregation
power at the lower temperature increased the domain spacing, whereas
a storage shear modulus (<i>G</i>′) showed liquid-like
behavior (<i>G</i>′<i>∝ ω</i><sup>2</sup>) at low frequencies (ω < 0.2 s<sup>–1</sup>) in a terminal zone and a shoulder at ω ∼ 1 s<sup>–1</sup>. The shoulder shifted toward the smaller ω region, arising
from dissociation of the PS block from the solvent. Once BCC lattice
structures of spherical microdomains formed, grains eventually grew
in size up to ca. 2.5 μm with a large size-distribution as revealed
by the 2d-SAXS with spot-like scatterings, whereas <i>G</i>′ in the terminal region increased, arising from the increase
in correlation length of the spherical microdomains. Eventually, the <i>G</i>′ showed plateau at lower frequencies at ω
< 0.2 s<sup>–1</sup>, indicating that the BCC lattice of
spheres with long-range order (grain stuructures) was percolated throughout
the solution. The number of the grains still continued to increase
at the cost of spherical microdomains in the lattice disordered state,
which caused the further increase in <i>G</i>′ at
the plateau until the end of the ordering process of the BCC structure