The controllable of BODIPY dimers without installing blocking groups as both fluorescence and singlet oxygen generators

Abstract We compared a range of BODIPY dimer derivatives without installing blocking groups by optimizing geometry structures and analyzing energies, frontier molecular orbitals, C hole& C ele map, electron density difference, spin‐orbit coupling (SOC) matrix and decay rate constants from excite...

Full description

Saved in:
Bibliographic Details
Published inSmart molecules (Print)
Main Authors Cao, Jianfang, Zhang, Tianci, Chen, Xinyu, Ma, Xue, Fan, Jiangli
Format Journal Article
LanguageEnglish
Published 21.07.2024
Online AccessGet full text

Cover

Loading…
More Information
Summary:Abstract We compared a range of BODIPY dimer derivatives without installing blocking groups by optimizing geometry structures and analyzing energies, frontier molecular orbitals, C hole& C ele map, electron density difference, spin‐orbit coupling (SOC) matrix and decay rate constants from excited states. The dihedral angles of the β ‐ β ‐linked BODIPY dimer and the α ‐ α ‐linked BODIPY dimer tend to flatten in the T 1 state, which is detrimental to the occurrence of the intersystem crossing (ISC). Conversely, the dihedral angle of the meso ‐ β ‐linked BODIPY dimer, the meso ‐ meso ‐linked BODIPY dimer and α ‐ γ ‐linked BODIPY dimer is within the range of 125°–143° in the T 1 state, facilitating ISC and the generation of singlet oxygen. Notably, the transition from S 1 to S 0 involving lowest unoccupied molecular orbital to highest occupied molecular orbital with long‐wavelength emission and moderate oscillator strength underpins the remarkable long emission peaks observed experimentally for α ‐ γ ‐linked BODIPY dimer. Moreover, the apparent SOC matrix enhances the ISC process, resulting in a respectable efficiency in generating singlet oxygen for this dimer. In meso ‐ β ‐linked BODIPY, meso ‐ meso ‐linked BODIPY, and α ‐ γ ‐linked BODIPY, the S 1 →T 1 process is characterized by a significant charge transfer, specifically transitioning from the 1 CT state to the 3 LE state, indicative of a spin‐orbit charge transfer ISC (SOCT‐ISC) mechanism. The ability to regulate the photosensitivity of BODIPY dimers by adjusting the dihedral angle between the two units in the T 1 state unveils new avenues for designing high‐performance photosensitizers for both therapeutic and imaging applications.
ISSN:2751-4587
2751-4595
DOI:10.1002/smo.20240023