Crystals (Feb 2019)

High-Temperature Cooperative Spin Crossover Transitions and Single-Crystal Reflection Spectra of [Fe<sup>III</sup>(qsal)<sub>2</sub>](CH<sub>3</sub>OSO<sub>3</sub>) and Related Compounds

  • Kazuyuki Takahashi,
  • Kaoru Yamamoto,
  • Takashi Yamamoto,
  • Yasuaki Einaga,
  • Yoshihito Shiota,
  • Kazunari Yoshizawa,
  • Hatsumi Mori

DOI
https://doi.org/10.3390/cryst9020081
Journal volume & issue
Vol. 9, no. 2
p. 81

Abstract

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New Fe(III) compounds from qsal ligand, [Fe(qsal)2](CH3OSO3) (1) and [Fe(qsal)2](CH3SO3)·CH3OH (3), along with known compound, [Fe(qsal)2](CF3SO3) (2), were obtained as large well-shaped crystals (Hqsal = N-(8-quinolyl)salicylaldimine). The compounds 1 and 2 were in the low-spin (LS) state at 300 K and exhibited a cooperative spin crossover (SCO) transition with a thermal hysteresis loop at higher temperatures, whereas 3 was in the high-spin (HS) state below 300 K. The optical conductivity spectra for 1 and 3 were calculated from the single-crystal reflection spectra, which were, to the best of our knowledge, the first optical conductivity spectra of SCO compounds. The absorption bands for the LS and HS [Fe(qsal)2] cations were assigned by time-dependent density functional theory calculations. The crystal structures of 1 and 2 consisted of a common one-dimensional (1D) array of the [Fe(qsal)2] cation, whereas that of 3 had an unusual 1D arrangement by π-stacking interactions which has never been reported. The crystal structures in the high-temperature phases for 1 and 2 indicate that large structural changes were triggered by the motion of counter anions. The comparison of the crystal structures of the known [Fe(qsal)2] compounds suggests the significant role of a large non-spherical counter-anion or solvate molecule for the total lattice energy gain in the crystal of a charged complex.

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