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Interplay between spin crossover and proton migration along short strong hydrogen bonds

The iron(ii) salt [Fe(bpp)(2)](isonicNO)(2)·HisonicNO·5H(2)O (1) (bpp = 2,6-bis(pyrazol-3-yl)pyridine; isonicNO = isonicotinate N-oxide anion) undergoes a partial spin crossover (SCO) with symmetry breaking at T(1) = 167 K to a mixed-spin phase (50% high-spin (HS), 50% low-spin (LS)) that is metasta...

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Detalles Bibliográficos
Autores principales: Jornet-Mollá, Verónica, Giménez-Saiz, Carlos, Cañadillas-Delgado, Laura, Yufit, Dmitry S., Howard, Judith A. K., Romero, Francisco M.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8179063/
https://www.ncbi.nlm.nih.gov/pubmed/34163870
http://dx.doi.org/10.1039/d0sc04918b
Descripción
Sumario:The iron(ii) salt [Fe(bpp)(2)](isonicNO)(2)·HisonicNO·5H(2)O (1) (bpp = 2,6-bis(pyrazol-3-yl)pyridine; isonicNO = isonicotinate N-oxide anion) undergoes a partial spin crossover (SCO) with symmetry breaking at T(1) = 167 K to a mixed-spin phase (50% high-spin (HS), 50% low-spin (LS)) that is metastable below T(2) = 116 K. Annealing the compound at lower temperatures results in a 100% LS phase that differs from the initial HS phase in the formation of a hydrogen bond (HB) between two water molecules (O4W and O5W) of crystallisation. Neutron crystallography experiments have also evidenced a proton displacement inside a short strong hydrogen bond (SSHB) between two isonicNO anions. Both phenomena can also be detected in the mixed-spin phase. 1 undergoes a light-induced excited-state spin trapping (LIESST) of the 100% HS phase, with breaking of the O4W⋯O5W HB and the onset of proton static disorder in the SSHB, indicating the presence of a light-induced activation energy barrier for proton motion. This excited state shows a stepped relaxation at T(1)(LIESST) = 68 K and T(2)(LIESST) = 76 K. Photocrystallography measurements after the first relaxation step reveal a single Fe site with an intermediate geometry, resulting from the random distribution of the HS and LS sites throughout the lattice.