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Synthesis of a Borylated Ibuprofen Derivative Through Suzuki Cross-Coupling and Alkene Boracarboxylation Reactions
Published on: November 30, 2022
C-H Borylation/Cross-Coupling Forms Twisted Donor-Acceptor Compounds Exhibiting Donor-Dependent Delayed Emission
Daniel L Crossley1, Pakapol Kulapichitr1, James E Radcliffe1
1School of Chemistry, The University of Manchester, Oxford Road, Manchester, M13 9PL, UK.
Researchers developed a new method for synthesizing twisted donor-acceptor compounds using C-H borylation and Suzuki-Miyaura cross-coupling. Long-lifetime emission was observed with triphenylamine donors due to specific excited state energy gaps.
Area of Science:
- Organic Chemistry
- Materials Science
- Photophysics
Background:
- Donor-acceptor (D-A) compounds are crucial in organic electronics.
- Developing efficient synthetic routes to complex D-A architectures remains a challenge.
- Understanding structure-property relationships is key for tuning optoelectronic properties.
Purpose of the Study:
- To develop a facile synthetic strategy for twisted D-A compounds.
- To explore the synthesis of borylated D-A and D-A-D systems.
- To investigate the photophysical properties and structure-dependent emission characteristics.
Main Methods:
- Benzothiadiazole (BT) directed C-H borylation using BCl3.
- B-Cl hydrolysis and Suzuki-Miyaura cross-coupling reactions.
- Photophysical characterization (emission studies) and computational modeling (excited state analysis).
Main Results:
- Facile access to twisted D-A compounds via sequential C-H borylation and cross-coupling.
- Synthesis of borylated twisted D-A and D-A-D compounds.
- Long-lifetime emission observed exclusively with triphenylamine donors.
- Computational analysis identified S1/T2 and T1 excited state energy gaps as critical for emission properties.
Conclusions:
- The developed synthetic route offers efficient access to novel twisted D-A architectures.
- Triphenylamine donors are essential for achieving long-lifetime emission in these systems.
- The energy gap between specific excited states dictates the observed photophysical behavior.
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