High‐Energy Long‐Lived Mixed Frenkel–Charge‐Transfer Excitons: From Double Stranded (AT)<sub><i>n</i></sub> to Natural DNA

  • Ignacio Vayá
    LIDYL, CEA, CNRS Université Paris Saclay 91191 Gif-sur-Yvette France
  • Johanna Brazard
    LIDYL, CEA, CNRS Université Paris Saclay 91191 Gif-sur-Yvette France
  • Miquel Huix‐Rotllant
    LIDYL, CEA, CNRS Université Paris Saclay 91191 Gif-sur-Yvette France
  • Arun K. Thazhathveetil
    Department of Chemistry Northwestern University Evanston Illinois 60208 USA
  • Frederick D. Lewis
    Department of Chemistry Northwestern University Evanston Illinois 60208 USA
  • Thomas Gustavsson
    LIDYL, CEA, CNRS Université Paris Saclay 91191 Gif-sur-Yvette France
  • Irene Burghardt
    Institut für Physikalische und Theoretische Chemie Goethe-Universität Max-von-Laue-Str. 7 60438 Frankfurt am Main Germany
  • Roberto Improta
    Istituto Biostrutture e Bioimmagini-Consiglio Nazionale delle Ricerche Via mezzocannone 16 80136 Napoli Italy
  • Dimitra Markovitsi
    LIDYL, CEA, CNRS Université Paris Saclay 91191 Gif-sur-Yvette France

説明

<jats:title>Abstract</jats:title><jats:p>The electronic excited states populated upon absorption of UV photons by DNA are extensively studied in relation to the UV‐induced damage to the genetic code. Here, we report a new unexpected relaxation pathway in adenine–thymine double‐stranded structures (AT)<jats:sub><jats:italic>n</jats:italic></jats:sub>. Fluorescence measurements on (AT)<jats:sub><jats:italic>n</jats:italic></jats:sub> hairpins (six and ten base pairs) and duplexes (20 and 2000 base pairs) reveal the existence of an emission band peaking at approximately 320 nm and decaying on the nanosecond time scale. Time‐dependent (TD)‐DFT calculations, performed for two base pairs and exploring various relaxation pathways, allow the assignment of this emission band to excited states resulting from mixing between Frenkel excitons and adenine‐to‐thymine charge‐transfer states. Emission from such high‐energy long‐lived mixed (HELM) states is in agreement with their fluorescence anisotropy (0.03), which is lower than that expected for π–π* states (≥0.1). An increase in the size of the system quenches π–π* fluorescence while enhancing HELM fluorescence. The latter process varies linearly with the hypochromism of the absorption spectra, both depending on the coupling between π–π* and charge‐transfer states. Subsequently, we identify the common features between the HELM states of (AT)<jats:sub><jats:italic>n</jats:italic></jats:sub> structures with those reported previously for alternating (GC)<jats:sub><jats:italic>n</jats:italic></jats:sub>: high emission energy, low fluorescence anisotropy, nanosecond lifetimes, and sensitivity to conformational disorder. These features are also detected for calf thymus DNA in which HELM states could evolve toward reactive π–π* states, giving rise to delayed fluorescence.</jats:p>

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