TY - JOUR
T1 - Phase behavior in thin films of weakly segregated block copolymer/homopolymer blends
AU - Hong, Jia Wen
AU - Chang, Jung Hong
AU - Chang, Iris Ching Ya
AU - Sun, Ya Sen
N1 - Publisher Copyright:
© The Royal Society of Chemistry 2021.
PY - 2021/10/28
Y1 - 2021/10/28
N2 - We have demonstrated the phase behavior of substrate-supported films of a symmetric weakly segregated polystyrene-block-poly (methyl methacrylate), P(S-b-MMA), block copolymer and its blends with homopolymer polystyrene (PS) at different compositions. Upon increasing the content of added PS in the blends, lamellae (L), perforated layers (PL), double gyroid (DG) and cylinders (C) are obtained in sequence for films. Among these nanodomains, PL and DG only exist in a narrowϕPSregion (ϕPSdenotes the volume fraction of PS). AtϕPS= 64%, tuning film thickness and annealing temperature can produce parallel PL or DG with {121}DGlattice planes being parallel to the substrate surface. The effects of annealing temperature and film thickness on the formation of PL and DG are examined. In thin films withn≈ 3 (ndenotes the ratio of initial film thickness to inter-domain spacing), the PL phase solely exists regardless of temperature. However, for thick films withn≈ 6 and 10, thermal annealing at the most accessible temperature produces films containing both PL and DG of various fractions, but a low temperature tends to favor a greater fraction of PL. The PL phase becomes the only discernible phase if thick films are shortly annealed at 230 °C.
AB - We have demonstrated the phase behavior of substrate-supported films of a symmetric weakly segregated polystyrene-block-poly (methyl methacrylate), P(S-b-MMA), block copolymer and its blends with homopolymer polystyrene (PS) at different compositions. Upon increasing the content of added PS in the blends, lamellae (L), perforated layers (PL), double gyroid (DG) and cylinders (C) are obtained in sequence for films. Among these nanodomains, PL and DG only exist in a narrowϕPSregion (ϕPSdenotes the volume fraction of PS). AtϕPS= 64%, tuning film thickness and annealing temperature can produce parallel PL or DG with {121}DGlattice planes being parallel to the substrate surface. The effects of annealing temperature and film thickness on the formation of PL and DG are examined. In thin films withn≈ 3 (ndenotes the ratio of initial film thickness to inter-domain spacing), the PL phase solely exists regardless of temperature. However, for thick films withn≈ 6 and 10, thermal annealing at the most accessible temperature produces films containing both PL and DG of various fractions, but a low temperature tends to favor a greater fraction of PL. The PL phase becomes the only discernible phase if thick films are shortly annealed at 230 °C.
UR - http://www.scopus.com/inward/record.url?scp=85117700908&partnerID=8YFLogxK
U2 - 10.1039/d1sm01005k
DO - 10.1039/d1sm01005k
M3 - 期刊論文
C2 - 34586138
AN - SCOPUS:85117700908
SN - 1744-683X
VL - 17
SP - 9189
EP - 9197
JO - Soft Matter
JF - Soft Matter
IS - 40
ER -