2015
DOI: 10.1088/1742-6596/640/1/012010
|View full text |Cite
|
Sign up to set email alerts
|

Kinetics of directed self-assembly of block copolymers on chemically patterned substrates

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
12
0

Year Published

2016
2016
2021
2021

Publication Types

Select...
9

Relationship

3
6

Authors

Journals

citations
Cited by 15 publications
(14 citation statements)
references
References 46 publications
2
12
0
Order By: Relevance
“…On the basis of previous studies, , these fully aligned lamellar domains should never relapse to a defective state due to the large difference in free energy between the aligned and nonaligned states, and these grains will gradually grow until defects are annihilated. The initially independent development of registered structures at the bottom and randomly oriented structures at the top was similar to the simulations results by Edwards et al and Müller et al , However, the stitch morphology was not observed in those studies, possibly because they used 1:1 DSA instead of the 3:1 pattern multiplication in this work.…”
Section: Resultssupporting
confidence: 90%
“…On the basis of previous studies, , these fully aligned lamellar domains should never relapse to a defective state due to the large difference in free energy between the aligned and nonaligned states, and these grains will gradually grow until defects are annihilated. The initially independent development of registered structures at the bottom and randomly oriented structures at the top was similar to the simulations results by Edwards et al and Müller et al , However, the stitch morphology was not observed in those studies, possibly because they used 1:1 DSA instead of the 3:1 pattern multiplication in this work.…”
Section: Resultssupporting
confidence: 90%
“…To confirm this point, we perform the SCMF simulations to estimate the lifetime t f of D1 and D2 defects as a function of χ N . t f in units of the relaxation time τ = R g 0 2 / D , where D and R g 0 are the diffusion constant and the radius of gyration of an undisturbed particle-based polymer chain with N segments in the disordered melt, respectively, is estimated with eight independent samples by simulation as shown in Figure c. , Since the lifetime of a defect is protracted by its free-energy barrier, t f ∝ τ exp­(Δ F b / k B T ) with Δ F b / k B T = b 2 ρ 0 L z Δ F ̃ b , it increases rapidly with χ N . , The plot of ln­( t f /τ) with respect to Δ F b / k B T in the inset of Figure c shows an approximate linear relationship. Obviously, the annihilating process of D2 of AB 2 is significantly slower than that of D1 of AB even in the situation of the equal free-energy barrier.…”
Section: Resultsmentioning
confidence: 99%
“…Equipped with the method, we have studied the specific example of DSA of diblock copolymer thin films with a threefold density multiplication . In contrast to 1:1 pattern replication, where the guiding pattern at the bottom surface gives rise to the formation of an ordered and registered grain in its vicinity that vertically expands and simply pushes misaligned structures out of the top surface (see Supporting Movie M0), , the kinetics of structure formation in the case of density multiplication is significantly more complex. Quite dramatically, the equilibrium free energy bears little correlation with the statistical likelihood of observing a given structure.…”
Section: Discussionmentioning
confidence: 99%