4.8 Article

Bifurcation of excited state trajectories toward energy transfer or electron transfer directed by wave function symmetry

出版社

NATL ACAD SCIENCES
DOI: 10.1073/pnas.2018521118

关键词

wave function symmetry; excited state electronic coupling; photoinduced mixed valence; energy transfer; electron transfer

资金

  1. University of Buenos Aires [UBACyT 20020130100534BA]
  2. CONICET [PIP 112-20150100394CO]
  3. ANPCyT [PICT 2013 00069, PICT 2018-00924]

向作者/读者索取更多资源

This work investigates the concept of engineering differential wave function overlap between excited states within a molecular chromophore to control excited state wave function symmetries, which leads to differential orbital overlap and low-energy trajectories within the excited state surface. By exploring two donor-acceptor assemblies, it was found that visible light absorption can prepare excited states with different wave function symmetry, allowing for energy transfer and backelectron transfer. The presence of kinetic barriers prevents excited state equilibration, providing a strategy to avoid energy dissipation in energy conversion or photoredox catalytic schemes.
This work explores the concept that differential wave function overlap between excited states can be engineered within a molecular chromophore. The aim is to control excited state wave function symmetries, so that symmetry matches or mismatches result in differential orbital overlap and define low-energy trajectories or kinetic barriers within the excited state surface, that drive excited state population toward different reaction pathways. Two donor-acceptor assemblies were explored, where visible light absorption prepares excited states of different wave function symmetry. These states could be resolved using transient absorption spectroscopy, thanks to wave function symmetry-specific photoinduced optical transitions. One of these excited states undergoes energy transfer to the acceptor, while another undertakes a backelectron transfer to restate the ground state. This differential behavior is possible thanks to the presence of kinetic barriers that prevent excited state equilibration. This strategy can be exploited to avoid energy dissipation in energy conversion or photoredox catalytic schemes.

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