

FOLLOWUS
a.Department of Physics, Taizhou University, Taizhou 318000, China
b.Key Laboratory of Computational Physical Science, Fudan University, Shanghai 200433, China
c.Department of Chemistry, Zhejiang Sci-Tech University, Hangzhou 310018, China
d.Faculty of Materials Science and Chemical Engineering, Ningbo University, Ningbo 315211, China
zhaobin007@tzc.edu.cn (B.Z.)
xuyuci@nbu.edu.cn (Y.C.X.)
Received:30 November 2020,
Revised:2021-1-5,
Accepted:15 January 2021,
Online First:30 April 2021,
Published:14 May 2021
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Zhao, B.; Liu, M. J.; Wang, C.; Chen, Y. C.; Xu, Y. C. Enlarged stable phase region of hybrid lamella-sphere phase enabled by A1B1A2(B2),
Bin Zhao, Mei-Jiao Liu, Chao Wang, et al. Enlarged Stable Phase Region of Hybrid Lamella-sphere Phase Enabled by A1B1A2(B2)
Zhao, B.; Liu, M. J.; Wang, C.; Chen, Y. C.; Xu, Y. C. Enlarged stable phase region of hybrid lamella-sphere phase enabled by A1B1A2(B2),
Bin Zhao, Mei-Jiao Liu, Chao Wang, et al. Enlarged Stable Phase Region of Hybrid Lamella-sphere Phase Enabled by A1B1A2(B2)
Hybrid nanostructures possess a great potential for application in advanced nanotechnologies due to the anisotropic properties from different nanophases. Our previous work demonstrated that a linear A
1
B
1
A
2
B
2
tetrablock copolymer of symmetric overall volume fraction can self-assemble into a hybrid lamella-sphere (LS) structure by tuning the relative length of the two A-blocks through self-consistent field theory (SCFT)
where the spherical and the lamellar domains are mainly composed of the long A
1
- and short A
2
-blocks
respectively. However
the phase region of LS is limited. In order to expand the stable region of LS
we change the linear A
1
B
1
A
2
B
2
copolymer to a branched A
1
B
1
A
2
(B
2
)
m
copolymer resulting in an increase of the local spontaneous curvature between A
2
- and B
2
-blocks. We examine the impact of the branching number
m
of B
2
-block on the stable region of LS in the phase diagram with respect to
f
A1
and
χN
for fixed
f
B
=0.5 and
f
B1
=0.26
and find that
m
=2 expands the LS region significantly in contrast to the linear architecture. On the other hand
the stability window of LS does not change notably when
m
=2 is increased to 3 in our calculated parameter space.
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