Abstract
The efficient preparation of single-crystalline ionic polymers and fundamental understanding of their structure-property relationships at the molecular level remains a challenge in chemistry and materials science. Here, we describe the single-crystal structure of a highly ordered polycationic polymer (polyelectrolyte) and its proton conductivity. The polyelectrolyte single crystals can be prepared on a gram-scale in quantitative yield, by taking advantage of an ultraviolet/sunlight-induced topochemical polymerization, from a tricationic monomer- A self-complementary building block possessing a preorganized conformation. A single-crystal-to-single-crystal photopolymerization was revealed unambiguously by in situ single-crystal X-ray diffraction analysis, which was also employed to follow the progression of molecular structure from the monomer, to a partially polymerized intermediate, and, finally, to the polymer itself. Collinear polymer chains are held together tightly by multiple Coulombic interactions involving counterions to form two-dimensional lamellar sheets (1 nm in height) with sub-nanometer pores (5 Å). The polymer is extremely stable under 254 nm light irradiation and high temperature (above 500 K). The extraordinary mechanical strength and environmental stability-in combination with its impressive proton conductivity (âˆ3 × 10-4 S cm-1)-endow the polymer with potential applications as a robust proton-conducting material. By marrying supramolecular chemistry with macromolecular science, the outcome represents a major step toward the controlled synthesis of single-crystalline polyelectrolyte materials with perfect tacticity.
Original language | English |
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Pages (from-to) | 6180-6187 |
Number of pages | 8 |
Journal | Journal of the American Chemical Society |
Volume | 142 |
Issue number | 13 |
DOIs | |
State | Published - Apr 1 2020 |
Funding
We thank Drs. Charlotte L. Stern and Christos D. Malliakas for discussions relating to the SCXRD and PXRD. We thank Dr. Xiaobing Hu and Xinyi Gong for discussions about HRTEM. We also thank Dr. Zhiqiang Pei for discussions about the setup of the LED light. The authors gratefully thank Northwestern University for supporting this research. We made use of the facility of Integrated Molecular Structure Education and Research Center (IMSERC) and Northwestern University’s NUANCE Center. M.J. and M.R. thank the W.M. Keck Center for Nanoscale Optofluidics, the California Institute for Quantitative Biosciences (QB3), and the Army Research Office under award number W911NF-17-1-0460 for equipment and facilities support. O.K.F. acknowledges the financial support from the U.S. Department of Energy, National Nuclear Security Administration under Award Number DE-NA0003763. M.R.R. acknowledges the U.S. Department of Energy Office of Science (Basic Energy Sciences) for research funding and the National Energy Research Scientific Computing Center (NERSC), a U.S. Department of Energy Office of Science User Facility operated under Contract No. DE-AC02-05CH11231, for access to supercomputing resources. M.R.R. also acknowledges computing resources provided by STFC Scientific Computing Department’s SCARF cluster. R.Q.S. acknowledges support from the U.S. Department of Energy under Award DE-FG02-08ER15967. Z.L. acknowledges the Supercomputer Center of Westlake University and financial support from the National Natural Science Foundation of China under Award Number 21971211.
Funders | Funder number |
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NERSC | DE-FG02-08ER15967 |
National Energy Research Scientific Computing Center | |
U.S. Department of Energy Office of Science | |
W.M. Keck Center for Nanoscale Optofluidics | |
Westlake University | |
U.S. Department of Energy | |
Army Research Office | W911NF-17-1-0460 |
Basic Energy Sciences | |
National Nuclear Security Administration | DE-NA0003763 |
Northwestern University | |
California Institute for Quantitative Biosciences | |
National Natural Science Foundation of China | 21971211 |