Highly fluorescent purine-containing conjugated copolymers with tailored optoelectronic properties

C. Elizabeth O'Connell, Sina Sabury, J. Elias Jenkins, Graham S. Collier, Bobby G. Sumpter, Brian K. Long, S. Michael Kilbey

Research output: Contribution to journalArticlepeer-review

5 Scopus citations

Abstract

Conjugated copolymers containing electron donor and acceptor units in their main chain have emerged as promising materials for organic electronic devices due to their tunable optoelectronic properties. Herein, we describe the use of direct arylation polymerization to create a series of fully π-conjugated copolymers containing the highly tailorable purine scaffold as a key design element. To create efficient coupling sites, dihalopurines are flanked by alkylthiophenes to create a monomer that is readily copolymerized with a variety of conjugated comonomers, ranging from electron-donating 3,4-dihydro-2H-thieno[3,4-b][1,4]dioxepine to electron-accepting 4,7-bis(5-bromo-3-hexylthiophen-2-yl)benzo[c][1,2,5]thiadiazole. The comonomer choice and electronic nature of the purine scaffold allow the photophysical properties of the purine-containing copolymers to be widely varied, with optical bandgaps ranging from 1.96-2.46 eV, and photoluminescent quantum yields as high as ϕ = 0.61. Frontier orbital energy levels determined for the various copolymers using density functional theory tight binding calculations track with experimental results, and the geometric structures of the alkylthiophene-flanked purine monomer and its copolymer are found to be nearly planar. The utility of direct arylation polymerization and intrinsic tailorability of the purine scaffold highlight the potential of these fully conjugated polymers to establish structure-property relationships based on connectivity pattern and comonomer type, which may broadly inform efforts to advance purine-containing conjugated copolymers for various applications.

Original languageEnglish
Pages (from-to)4921-4933
Number of pages13
JournalPolymer Chemistry
Volume13
Issue number34
DOIs
StatePublished - Aug 12 2022

Funding

This work was sponsored in part by the US Department of Energy's Office of Energy Efficiency and Renewable Energy (EERE) under the award number DE-EE0009177 provided to the University of Tennessee - Oak Ridge Innovation Institute (UT-ORII). SMK and BKL also acknowledge support from the National Science Foundation (Award # 2204396). CEO and SS acknowledge support in part from the UT-ORII Science Alliance Graduate Advancement, Training, and Education (GATE) program. Dr Gabriel Goenaga is acknowledged with thanks for assistance with cyclic voltammetry measurements. DFT and DFTB calculations were performed at the Center for Nanophase Materials Sciences, a US Department of Energy Office of Science User Facility. This work was sponsored in part by the US Department of Energy's Office of Energy Efficiency and Renewable Energy (EERE) under the award number DE-EE0009177 provided to the University of Tennessee – Oak Ridge Innovation Institute (UT-ORII). SMK and BKL also acknowledge support from the National Science Foundation (Award # 2204396). CEO and SS acknowledge support in part from the UT-ORII Science Alliance Graduate Advancement, Training, and Education (GATE) program. Dr Gabriel Goenaga is acknowledged with thanks for assistance with cyclic voltammetry measurements. DFT and DFTB calculations were performed at the Center for Nanophase Materials Sciences, a US Department of Energy Office of Science User Facility.

FundersFunder number
Center for Nanophase Materials Sciences
Oak Ridge Innovation Institute
UT-ORII
UT-ORII Science Alliance
University of Tennessee - Oak Ridge Innovation Institute
National Science Foundation2204396
U.S. Department of Energy
Office of Science
Office of Energy Efficiency and Renewable EnergyDE-EE0009177
University of Tennessee

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