Photoelectron Imaging Spectroscopy of C <sub>6</sub> Cl <i> <sub>x</sub> </i> F <sub> 6– <i>x</i> </sub> <sup>–</sup> ( <i>x</i> = 2, 3, 5) and C <sub>2</sub> Cl <sub>4</sub> <sup>–</sup> Anions: Charge Localization or Delocalization─That Is the Ques
New photoelectron (PE) spectra of C<sub>6</sub>Cl<sub><i>x</i></sub>F<sub>6-<i>x</i></sub><sup>-</sup> (<i>x</i> = 2, 3, 5) are presented and compared with previously reported PE spectra of C<sub>6</sub>F<sub>6</sub><sup>-</sup> and C<sub>6</sub>ClF<sub>5</sub><sup>-</sup>, along with the known properties of C<sub>6</sub>Cl<sub>6</sub><sup>-</sup>. Based on a recent theoretical study [<i>J. Phys. Chem. A</i> <b>2024,</b> <i>128,</i> 8072-8079], anions of the mixed perchlorofluorobenzenes have competing molecular and electronic structures: one in which the electron is localized in a single C-Cl σ* orbital, resulting in a structure with a uniquely elongated C-Cl bond, and the other in which the excess charge is more delocalized, resulting in a more symmetric anion. In all cases, the experimental PE spectra are consistent with the former, with the exception of C<sub>6</sub>Cl<sub>5</sub>F<sup>-</sup>, the spectrum of which is not consistent with calculations on either structure. The adiabatic electron affinities of the neutrals are difficult to ascertain from the anion PE spectra because of vanishingly small signal near the origin. However, the vertical detachment energies are determined to be 3.20(10) eV for C<sub>6</sub>Cl<sub>2</sub>F<sub>4</sub><sup>-</sup>, 3.09(5) eV for C<sub>6</sub>Cl<sub>3</sub>F<sub>3</sub><sup>-</sup>, and 1.85(10) eV for C<sub>6</sub>Cl<sub>5</sub>F<sup>-</sup>. The VDEs of C<sub>6</sub>Cl<sub>2</sub>F<sub>4</sub><sup>-</sup> and C<sub>6</sub>Cl<sub>3</sub>F<sub>3</sub><sup>-</sup> are similar to the previously reported VDE of C<sub>6</sub>ClF<sub>5</sub><sup>-</sup>, 2.95 eV [<i>J. Phys. Chem. A</i> <b>2024,</b> <i>128,</i> 5646-5658], and significantly higher than the previously reported VDE determined from the PE spectrum of C<sub>6</sub>F<sub>6</sub><sup>-</sup>, 1.60 eV, measured on the same instrument [<i>J. Phys. Chem. A</i> <b>2023,</b> <i>127,</i> 556-8565]. To further benchmark the computational methods and gain insights into the relationship between the anionic structures in which the excess charge is localized in a single C-Cl σ* orbital and the delocalized structure, we measured the PE spectrum C<sub>2</sub>Cl<sub>4</sub><sup>-</sup>, which exhibited a VDE consistent with the computed structure in which the excess charge is localized in a single C-Cl σ* orbital, and which was the computed lowest energy structure of C<sub>2</sub>Cl<sub>4</sub><sup>-</sup>. We further explore the relationship between localized and delocalized structures in this molecular anion and C<sub>6</sub>Cl<sub>5</sub>F<sup>-</sup>.
Authors
- Caroline Chick Jarrold (ORCID: https://orcid.org/0000-0001-9725-4581)
- Thomas Sommerfeld (ORCID: https://orcid.org/0000-0001-8105-5414)
- Conor J. McGee (ORCID: https://orcid.org/0009-0007-8563-0720)
- Kristen Rose McGinnis (ORCID: https://orcid.org/0000-0001-8630-7166)
- Raegan M. Aiena
Institutions
- Southeastern Louisiana University (US)
- Indiana University Bloomington (US)
Publication Details
- Journal
- The Journal of Physical Chemistry A
- Published
- 2026-02-19
- DOI
- https://doi.org/10.1021/acs.jpca.6c00196
- Primary Topic
- Advanced Chemical Physics Studies
- Type
- article
- Field-Weighted Citation Impact
- 0.00