Structure and spin of the low- and high-spin states of Fe 2+ (phen) 3 studied by x-ray scattering and emission spectroscopy.

Autor: Kabanova V; X-ray Photon Science, Uppsala, MB 516, Sweden., Sander M; Paul Scherrer Institute, 5232 Villigen, Switzerland., Levantino M; European Synchrotron Radiation Facility, CS 40220 Grenoble Cédex 9, France., Kong Q; Synchrotron Soleil, L'Orme des Merisiers, 91190 Saint-Aubin, France., Canton S; Danmarks Tekniske Universitet, 2800 Lyngby, Denmark., Retegan M; European Synchrotron Radiation Facility, CS 40220 Grenoble Cédex 9, France., Cammarata M; European Synchrotron Radiation Facility, CS 40220 Grenoble Cédex 9, France., Lenzen P; SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA., Lawson LMD; Department of Physical Chemistry, Science II, CH-1211 Genève 4, Switzerland., Wulff M; European Synchrotron Radiation Facility, CS 40220 Grenoble Cédex 9, France.
Jazyk: angličtina
Zdroj: Structural dynamics (Melville, N.Y.) [Struct Dyn] 2024 Oct 23; Vol. 11 (5), pp. 054901. Date of Electronic Publication: 2024 Oct 23 (Print Publication: 2024).
DOI: 10.1063/4.0000254
Abstrakt: The structure and spin of photoexcited Fe 2+ (phen) 3 in water are examined by x-ray scattering and x-ray emission spectroscopy with 100 ps time resolution. Excitation of the low-spin (LS) ground state (GS) to the charge transfer state 1 MLCT * leads to the formation of a high-spin (HS) state that returns to the GS in 725 ps. Density functional theory (DFT) predicts a Fe-N bond elongation in HS by 0.19 Å in agreement with the scattering data. The angle between the ligands increases by 5.4° in HS, which allows the solvent to get 0.33 Å closer to Fe in spite of the expansion of the molecule. The rise in solvent temperature from the return of photoproducts to the GS is dominated by the formation dynamics of HS, 1 MLCT *  → HS, which is followed by a smaller rise from the HS → GS transition. The latter agrees with the 0.61 eV energy gap E(HS)-E(LS) calculated by DFT. However, the temperature rise from the 1 MLCT → HS transition is greater than expected, by a factor of 2.1, which is explained by the re-excitation of nascent HS * by the 1.2 ps pump pulse. This hypothesis is supported by optical spectroscopy measurements showing that the 1.2 ps long pump pulse activates the HS *  →  5 MLCT * channel, which is followed by the ultrafast return to HS * via intersystem crossing. Finally, the spins of the photoproducts are monitored by the K β emission and the spectra confirm that the spins of LS and HS states are 0 and 2, respectively.
Competing Interests: The authors have no conflicts to disclose.
(© 2024 Author(s).)
Databáze: MEDLINE
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