Feng Hongbo, Kash Benjamin, Yim Soonmin, Bagchi Kushal, Craig Gordon S W, Chen Wen, Rowan Stuart J, Nealey Paul F
Pritzker School of Molecular Engineering, University of Chicago, 5640 S. Ellis Avenue, Chicago, Illinois 60637, United States.
Department of Chemistry, University of Chicago, 5735 S. Ellis Avenue, Chicago, Illinois 60637, United States.
Langmuir. 2023 Oct 17;39(41):14688-14698. doi: 10.1021/acs.langmuir.3c02065. Epub 2023 Oct 2.
To form nanopatterns with self-assembled block copolymers (BCPs), it is desirable to have through-film domains that are oriented perpendicular to the substrate. The domain orientation is determined by the interfacial interactions of the BCP domains with the substrate and with the free surface. Here, we use thin films of two different sets of BCPs with A(B--C) architecture matched with a corresponding B--C copolymer nanocoating on the substrate to demonstrate two distinct wetting behaviors. The two sets of A(B--C) BCPs are made by using thiol-epoxy click chemistry to functionalize polystyrenepoly(glycidyl methacrylate) with trifluoroethanethiol (TFET) and either 2-mercaptopyridine (2MP) or methyl thioglycolate (MTG). For each set of BCPs, the composition ratio of the two thiols in the BCP (φ) is found that results in the two blocks of the modified BCP having equal surface energies (Δγ = 0). The corresponding B--C random copolymers were synthesized and used to modify the substrate, and the composition ratio (φ) values that resulted in the two blocks of the BCP having equal interfacial energy with the substrate (Δγ = 0) were determined with scanning electron microscopy. The correlation between each block's γ value and the interaction parameter, χ, is employed to explain the different wetting behaviors of the two sets of BCPs. For the thiol pair 2MP and TFET, the values of φ and φ that lead to Δγ = 0 and Δγ = 0, respectively, are significantly different. A similar difference was observed between the φ and φ values that lead to Δγ = 0 and Δγ = 0 for the BCPs made with the thiol pair MTG and TFET. In the latter case, for Δγ = 0 two windows of φ are identified, which can be explained by the thermodynamic interactions of the specific thiol pair and the A--(B--C) architecture.
为了用自组装嵌段共聚物(BCP)形成纳米图案,希望有垂直于基底取向的贯穿薄膜的畴。畴的取向由BCP畴与基底以及与自由表面的界面相互作用决定。在此,我们使用具有A(B - C)结构的两组不同BCP的薄膜,并在基底上匹配相应的B - C共聚物纳米涂层,以展示两种不同的润湿行为。这两组A(B - C)BCP是通过硫醇 - 环氧点击化学用三氟乙烷硫醇(TFET)和2 - 巯基吡啶(2MP)或硫代乙醇酸甲酯(MTG)对聚苯乙烯 - 聚(甲基丙烯酸缩水甘油酯)进行功能化制备的。对于每组BCP,发现BCP中两种硫醇的组成比(φ)使得改性BCP的两个嵌段具有相等的表面能(Δγ = 0)。合成了相应的B - C无规共聚物并用于改性基底,并用扫描电子显微镜确定导致BCP的两个嵌段与基底具有相等界面能(Δγ = 0)的组成比(φ)值。利用每个嵌段的γ值与相互作用参数χ之间的相关性来解释两组BCP不同的润湿行为。对于硫醇对2MP和TFET,分别导致Δγ = 0和Δγ = 0的φ和φ值有显著差异。在用硫醇对MTG和TFET制备的BCP中,导致Δγ = 0和Δγ = 0的φ和φ值之间也观察到类似差异。在后一种情况下,对于Δγ = 0,确定了两个φ窗口,这可以通过特定硫醇对的热力学相互作用和A - (B - C)结构来解释。