journal article·2023-10-17Open access

Wetting Behavior of A-block-(B-random-C) Copolymers with Equal Block Surface Energies on Surfaces Functionalized with B-random-C Copolymers

Hongbo Feng, Benjamin Kash, Soonmin Yim, Kushal Bagchi, Gordon S. W. Craig, Wen Chen, Stuart J. Rowan, Paul F. Nealey

Langmuir· Volume 39· Issue 41

Abstract

High Resolution Image Download MS PowerPoint Slide 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 -block- (B- random -C) architecture matched with a corresponding B- random -C copolymer nanocoating on the substrate to demonstrate two distinct wetting behaviors. The two sets of A -b- (B- r -C) BCPs are made by using thiol–epoxy click chemistry to functionalize polystyrene -block- poly(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 1 ) is found that results in the two blocks of the modified BCP having equal surface energies (Δγ air = 0). The corresponding B- r -C random copolymers were synthesized and used to modify the substrate, and the composition ratio (φ 2 ) values that resulted in the two blocks of the BCP having equal interfacial energy with the substrate (Δγ sub = 0) were determined with scanning electron microscopy. The correlation between each block’s γ sub 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 1 and φ 2 that lead to Δγ air = 0 and Δγ sub = 0, respectively, are significantly different. A similar difference was observed between the φ 1 and φ 2 values that lead to Δγ air = 0 and Δγ sub = 0 for the BCPs made with the thiol pair MTG and TFET. In the latter case, for Δγ sub = 0 two windows of φ 2 are identified, which can be explained by the thermodynamic interactions of the specific thiol pair and the A- b -(B- r -C) architecture.
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Research context

OpenAlex topics: Block Copolymer Self-Assembly · Advanced Polymer Synthesis and Characterization · Polymer Surface Interaction Studies

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

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

Chemical Sciences and Engineering Division, Argonne National Laboratory, 9700 S. Cass Avenue, Lemont, Illinois 60439, United States

Center for Molecular Engineering, Materials Science Division, Argonne National Laboratory, 9700 S. Cass Avenue, Lemont, Illinois 60439, United States

Funding

Center for Hierarchical Materials Design · Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource, National Science Foundation???s National Nanotechnology Coordinated Infrastructure · Office of Science, U.S. Department of Energy · University of Chicago Materials Research Science and Engineering Center, National Science Foundation · Soft Matter Characterization Facility of the University of Chicago

References (47)

Show source-provided references
1. 10.1021/acs.macromol.6b0235510.1021/acs.macromol.6b02355 ↗
2. 10.3390/polym910049410.3390/polym9100494 ↗
3. 10.1038/nature0177510.1038/nature01775 ↗
4. 10.1038/s41928-018-0147-410.1038/s41928-018-0147-4 ↗
5. 10.1117/1.JMM.11.3.03130210.1117/1.JMM.11.3.031302 ↗
6. 10.1038/s41563-022-01392-110.1038/s41563-022-01392-1 ↗
7. 10.1021/acsami.1c2283610.1021/acsami.1c22836 ↗
8. 10.1002/adma.20040076310.1002/adma.200400763 ↗
9. 10.1016/S1369-7021(10)70106-110.1016/S1369-7021(10)70106-1 ↗
10. 10.1021/mz300475g10.1021/mz300475g ↗
11. 10.1126/science.122604610.1126/science.1226046 ↗
12. 10.1038/nnano.2017.3410.1038/nnano.2017.34 ↗
13. 10.1038/s41467-019-10907-510.1038/s41467-019-10907-5 ↗
14. 10.1021/ja107309p10.1021/ja107309p ↗
15. 10.1021/ma00024a03010.1021/ma00024a030 ↗
16. 10.1039/C7ME00067G10.1039/C7ME00067G ↗
17. 10.1021/ma400735a10.1021/ma400735a ↗
18. 10.1021/acs.macromol.8b0127510.1021/acs.macromol.8b01275 ↗
19. 10.1021/ma902646t10.1021/ma902646t ↗
20. 10.1021/nn700164p10.1021/nn700164p ↗
21. 10.1021/nn305725q10.1021/nn305725q ↗
22. 10.1002/adma.20070186610.1002/adma.200701866 ↗
23. 10.1021/la991500c10.1021/la991500c ↗
24. 10.1021/nn900750w10.1021/nn900750w ↗
25. 10.1021/acs.macromol.9b0059710.1021/acs.macromol.9b00597 ↗
26. 10.1021/acsami.5b0220110.1021/acsami.5b02201 ↗
27. 10.1021/mz200016910.1021/mz2000169 ↗
28. 10.1002/app.1969.07013081510.1002/app.1969.070130815 ↗
29. 10.1080/002184670854458210.1080/0021846708544582 ↗
30. 10.1126/science.275.5305.145810.1126/science.275.5305.1458 ↗
31. 10.1016/S0079-6700(00)00012-510.1016/S0079-6700(00)00012-5 ↗
32. 10.1021/ma801839310.1021/ma8018393 ↗
33. 10.1038/s41598-017-10090-x10.1038/s41598-017-10090-x ↗
34. 10.1021/jp404702j10.1021/jp404702j ↗
35. 10.1051/jphys:019760037012014450010.1051/jphys:0197600370120144500 ↗
36. 10.1021/ma025718910.1021/ma0257189 ↗
37. 10.1021/la034974r10.1021/la034974r ↗
38. 10.1149/2.007403jss10.1149/2.007403jss ↗
39. 10.1021/acs.macromol.7b0013310.1021/acs.macromol.7b00133 ↗
40. 10.1021/ma100150j10.1021/ma100150j ↗
41. 10.1038/2735810.1038/27358 ↗
42. 10.1021/ma00064a03310.1021/ma00064a033 ↗
43. 10.1021/ma00188a01510.1021/ma00188a015 ↗
44. 10.1016/0032-3861(84)90207-610.1016/0032-3861(84)90207-6 ↗
45. 10.1021/acsmacrolett.2c0064510.1021/acsmacrolett.2c00645 ↗
46. 10.1002/adfm.20220683610.1002/adfm.202206836 ↗
47. 10.1021/ma800056s10.1021/ma800056s ↗