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Valence shell electronically excited states of norbornadiene and quadricyclane.
Cooper, Joseph C; Holland, David M P; Ingle, Rebecca A; Bonanomi, Matteo; Faccialà, Davide; De Oliveira, Nelson; Abid, Abdul R; Bachmann, Julien; Bhattacharyya, Surjendu; Borne, Kurtis; Bosch, Michael; Centurion, Martin; Chen, Keyu; Forbes, Ruaridh J G; Lam, Huynh V S; Odate, Asami; Rudenko, Artem; Venkatachalam, Anbu S; Vozzi, Caterina; Wang, Enliang; Weber, Peter M; Ashfold, Michael N R; Kirrander, Adam; Rolles, Daniel.
Afiliación
  • Cooper JC; Physical and Theoretical Chemistry Laboratory, Department of Chemistry, University of Oxford, Oxford OX1 3QZ, United Kingdom.
  • Holland DMP; STFC, Daresbury Laboratory, Warrington WA4 2DS, United Kingdom.
  • Ingle RA; Department of Chemistry, University College London, 20 Gordon Street, London WC1H 0AJ, United Kingdom.
  • Bonanomi M; Istituto di Fotonica e Nanotecnologie-CNR (CNR-IFN), Milano, Italy.
  • Faccialà D; Dipartimento di Fisica, Politecnico di Milano, Italy.
  • De Oliveira N; Istituto di Fotonica e Nanotecnologie-CNR (CNR-IFN), Milano, Italy.
  • Abid AR; Synchrotron Soleil, L'Orme des Merisiers, F-91192 Gif-sur-Yvette, France.
  • Bachmann J; J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA.
  • Bhattacharyya S; Nano and Molecular Systems Research Unit, University of Oulu, 90570 Oulu, Finland.
  • Borne K; Chemistry of Thin Film Materials, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erlangen, Germany.
  • Bosch M; J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA.
  • Centurion M; J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA.
  • Chen K; Chemistry of Thin Film Materials, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erlangen, Germany.
  • Forbes RJG; Department of Physics and Astronomy, University of Nebraska-Lincoln, Lincoln, Nebraska 68588, USA.
  • Lam HVS; J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA.
  • Odate A; Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.
  • Rudenko A; J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA.
  • Venkatachalam AS; Department of Chemistry, Brown University, Providence, Rhode Island 02912, USA.
  • Vozzi C; J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA.
  • Wang E; J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA.
  • Weber PM; Istituto di Fotonica e Nanotecnologie-CNR (CNR-IFN), Milano, Italy.
  • Ashfold MNR; Physical and Theoretical Chemistry Laboratory, Department of Chemistry, University of Oxford, Oxford OX1 3QZ, United Kingdom.
  • Kirrander A; J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas 66506, USA.
  • Rolles D; Department of Chemistry, Brown University, Providence, Rhode Island 02912, USA.
J Chem Phys ; 160(6)2024 Feb 14.
Article en En | MEDLINE | ID: mdl-38349638
ABSTRACT
The absolute photoabsorption cross sections of norbornadiene (NBD) and quadricyclane (QC), two isomers with chemical formula C7H8 that are attracting much interest for solar energy storage applications, have been measured from threshold up to 10.8 eV using the Fourier transform spectrometer at the SOLEIL synchrotron radiation facility. The absorption spectrum of NBD exhibits some sharp structure associated with transitions into Rydberg states, superimposed on several broad bands attributable to valence excitations. Sharp structure, although less pronounced, also appears in the absorption spectrum of QC. Assignments have been proposed for some of the absorption bands using calculated vertical transition energies and oscillator strengths for the electronically excited states of NBD and QC. Natural transition orbitals indicate that some of the electronically excited states in NBD have a mixed Rydberg/valence character, whereas the first ten excited singlet states in QC are all predominantly Rydberg in the vertical region. In NBD, a comparison between the vibrational structure observed in the experimental 11B1-11A1 (3sa1 ← 5b1) band and that predicted by Franck-Condon and Herzberg-Teller modeling has necessitated a revision of the band origin and of the vibrational assignments proposed previously. Similar comparisons have encouraged a revision of the adiabatic first ionization energy of NBD. Simulations of the vibrational structure due to excitation from the 5b2 orbital in QC into 3p and 3d Rydberg states have allowed tentative assignments to be proposed for the complex structure observed in the absorption bands between ∼5.4 and 7.0 eV.

Texto completo: 1 Banco de datos: MEDLINE Tipo de estudio: Prognostic_studies Idioma: En Año: 2024 Tipo del documento: Article

Texto completo: 1 Banco de datos: MEDLINE Tipo de estudio: Prognostic_studies Idioma: En Año: 2024 Tipo del documento: Article