Electronic Spectra of Cryogenically Cooled Na <sup>+</sup> -Pyrene and K <sup>+</sup> -Pyrene Complexes

The Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene complexes are investigated using two-color resonance enhanced photodissociation action spectroscopy in a cryogenic ion trap and through complementary density functional theory calculations. Both complexes are predicted to have π-bound structures in which the metal cation lies above the plane of the pyrene molecule, with calculated binding energies of 10570 and 8150 cm<sup>-1</sup>, respectively. Electronic spectra of Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene over the 26,000-33,000 cm<sup>-1</sup> range exhibit S<sub>1</sub>(B<sub>2u</sub>) ← S<sub>0</sub>(A<sub>g</sub>) and S<sub>2</sub>(B<sub>1u</sub>) ← S<sub>0</sub>(A<sub>g</sub>) band systems associated with excitation of the pyrene chromophore. The S<sub>1</sub>(B<sub>2u</sub>) ← S<sub>0</sub>(A<sub>g</sub>) band systems of Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene are dominated by progressions in Franck-Condon active a<sub>g</sub> vibrational modes, whereas transitions involving b<sub>3g</sub> vibrational modes, which are prominent in the spectrum of the bare pyrene molecule by virtue of Herzberg-Teller coupling, are relatively weak or absent altogether. The S<sub>1</sub> ← S<sub>0</sub> origin transitions are shifted to lower energy from the corresponding pyrene transitions by 273 cm<sup>-1</sup> for Na<sup>+</sup>-pyrene and 246 cm<sup>-1</sup> for K<sup>+</sup>-pyrene. Density functional theory calculations predict that an attached Na<sup>+</sup> or K<sup>+</sup> cation has a minor effect on the pyrene vibrational frequencies but enhances the intensity of the weak S<sub>1</sub> ← S<sub>0</sub> transition while reducing slightly the intensity of the S<sub>2</sub> ← S<sub>0</sub> transition, explaining the relative dominance of vibronic transitions involving a<sub>g</sub> vibrational modes in the S<sub>1</sub> ← S<sub>0</sub> spectra of Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene. The strong, broad S<sub>2</sub>(B<sub>1u</sub>) ← S<sub>0</sub>(A<sub>g</sub>) vibronic bands of Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene are also displaced to lower energy compared to the corresponding bands of the bare pyrene molecule.

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Journal
The Journal of Physical Chemistry A
Published
2025-10-14
DOI
https://doi.org/10.1021/acs.jpca.5c05782
Primary Topic
Advanced Chemical Physics Studies
Type
article
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article

Electronic Spectra of Cryogenically Cooled Na + -Pyrene and K + -Pyrene Complexes

Samuel J. P. Marlton, Patrick Watkins, Evan J. Bieske, Jack T. Buntine et al.
The Journal of Physical Chemistry A
Advanced Chemical Physics Studies
article

Electronic Spectra of Cryogenically Cooled Na + -Pyrene and K + -Pyrene Complexes

Samuel J. P. Marlton, Patrick Watkins, Evan J. Bieske, Jack T. Buntine, Chang Liu
article en

Abstract

The Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene complexes are investigated using two-color resonance enhanced photodissociation action spectroscopy in a cryogenic ion trap and through complementary density functional theory calculations. Both complexes are predicted to have π-bound structures in which the metal cation lies above the plane of the pyrene molecule, with calculated binding energies of 10570 and 8150 cm<sup>-1</sup>, respectively. Electronic spectra of Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene over the 26,000-33,000 cm<sup>-1</sup> range exhibit S<sub>1</sub>(B<sub>2u</sub>) ← S<sub>0</sub>(A<sub>g</sub>) and S<sub>2</sub>(B<sub>1u</sub>) ← S<sub>0</sub>(A<sub>g</sub>) band systems associated with excitation of the pyrene chromophore. The S<sub>1</sub>(B<sub>2u</sub>) ← S<sub>0</sub>(A<sub>g</sub>) band systems of Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene are dominated by progressions in Franck-Condon active a<sub>g</sub> vibrational modes, whereas transitions involving b<sub>3g</sub> vibrational modes, which are prominent in the spectrum of the bare pyrene molecule by virtue of Herzberg-Teller coupling, are relatively weak or absent altogether. The S<sub>1</sub> ← S<sub>0</sub> origin transitions are shifted to lower energy from the corresponding pyrene transitions by 273 cm<sup>-1</sup> for Na<sup>+</sup>-pyrene and 246 cm<sup>-1</sup> for K<sup>+</sup>-pyrene. Density functional theory calculations predict that an attached Na<sup>+</sup> or K<sup>+</sup> cation has a minor effect on the pyrene vibrational frequencies but enhances the intensity of the weak S<sub>1</sub> ← S<sub>0</sub> transition while reducing slightly the intensity of the S<sub>2</sub> ← S<sub>0</sub> transition, explaining the relative dominance of vibronic transitions involving a<sub>g</sub> vibrational modes in the S<sub>1</sub> ← S<sub>0</sub> spectra of Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene. The strong, broad S<sub>2</sub>(B<sub>1u</sub>) ← S<sub>0</sub>(A<sub>g</sub>) vibronic bands of Na<sup>+</sup>-pyrene and K<sup>+</sup>-pyrene are also displaced to lower energy compared to the corresponding bands of the bare pyrene molecule.

The Journal of Physical Chemistry AVol. 129(42)
The University of Melbourne (AU)
Openalex Percentile: Top 77%
Advanced Chemical Physics Studies
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