2017
DOI: 10.1007/s13233-017-5128-3
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Phase transition of block copolymer/homopolymer binary blends under 2D confinement

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Cited by 10 publications
(5 citation statements)
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“…Block copolymer (BCP) composed of chemically different blocks has attracted researchers over decades because the BCP generates fascinating self-assembled structures in nanoscale dimensions, and researchers have proposed many applications in nanotechnology, microelectronics, and clean energy. To correlate the physical properties of BCP with specific applications, it is imperative to attain fundamental understanding on the thermodynamic behaviors and phase transitions of BCPs in terms of their molecular parameters, as reported in many theoretical and experimental studies. In the case of symmetric A–B diblock copolymers, the BCPs undergo an order-to-disorder transition (ODT) from a lamellar structure to a disordered state upon decreasing segregation power of χ N , where χ and N represent the Flory–Huggins interaction parameter between two blocks and the overall degree of polymerization, respectively. , Thus, an ODT-type phase transition of BCPs similarly pertains to the upper critical solution transition (UCST) in the binary polymer blends, as the χ is inversely proportional to temperature ( T ). , …”
Section: Introductionmentioning
confidence: 99%
“…Block copolymer (BCP) composed of chemically different blocks has attracted researchers over decades because the BCP generates fascinating self-assembled structures in nanoscale dimensions, and researchers have proposed many applications in nanotechnology, microelectronics, and clean energy. To correlate the physical properties of BCP with specific applications, it is imperative to attain fundamental understanding on the thermodynamic behaviors and phase transitions of BCPs in terms of their molecular parameters, as reported in many theoretical and experimental studies. In the case of symmetric A–B diblock copolymers, the BCPs undergo an order-to-disorder transition (ODT) from a lamellar structure to a disordered state upon decreasing segregation power of χ N , where χ and N represent the Flory–Huggins interaction parameter between two blocks and the overall degree of polymerization, respectively. , Thus, an ODT-type phase transition of BCPs similarly pertains to the upper critical solution transition (UCST) in the binary polymer blends, as the χ is inversely proportional to temperature ( T ). , …”
Section: Introductionmentioning
confidence: 99%
“…We hypothesize that this phenomenon stems from local entropic penalties for each BCP layer within the onion-like PS- b -P4VP particles. In concentric lamellar structures, the BCP chains near the center experience stronger entropic penalties (i.e., stretching penalty) due to their higher local curvature . Thus, Au NPs may selectively segregate at the central domains of each layer to alleviate BCP chain stretching.…”
Section: Resultsmentioning
confidence: 99%
“…In concentric lamellar structures, the BCP chains near the center experience stronger entropic penalties (i.e., stretching penalty) due to their higher local curvature. 60 Thus, Au NPs may selectively segregate at the central domains of each layer to alleviate BCP chain stretching. The change in entropy between the domains of onion-like BCP particles gives the potential to control the number of Au NP layers (N) formed within the ALO particles.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…An interesting parameter that can be employed to influence BCP self-assembly is homopolymer additives. While homopolymer additives have been widely investigated for their ability to tune the self-assembly of BCP in the bulk [12][13][14] phase, studies that examine the effects of these homopolymer on corresponding systems in solution are comparatively limited [15]. A better understanding of homopolymer effects can allow more scientists to take advantage of this potentially facile approach to manipulate BCP morphology in solution for various applications.…”
Section: Introductionmentioning
confidence: 99%