High-Temperature Cooperative Spin Crossover Transitions and Single-Crystal Reflection Spectra of [FeIII(qsal)2](CH3OSO3) and Related Compounds

被引:12
|
作者
Takahashi, Kazuyuki [1 ]
Yamamoto, Kaoru [2 ]
Yamamoto, Takashi [3 ]
Einaga, Yasuaki [3 ]
Shiota, Yoshihito [4 ]
Yoshizawa, Kazunari [4 ]
Mori, Hatsumi [5 ]
机构
[1] Kobe Univ, Grad Sch Sci, Dept Chem, Nada Ku, 1-1 Rokkodai, Kobe, Hyogo 6578501, Japan
[2] Okayama Univ Sci, Dept Appl Phys, Kita Ku, 1-1 Ridaicho, Okayama, Okayama 7000005, Japan
[3] Keio Univ, Grad Sch Sci & Technol, Dept Chem, Kohoku Ku, 3-14-1 Hiyoshi, Yokohama, Kanagawa 2238522, Japan
[4] Kyushu Univ, Inst Mat Chem & Engn, Nishi Ku, 744 Motooka, Fukuoka, Fukuoka 8190395, Japan
[5] Univ Tokyo, Inst Solid State Phys, 5-1-5 Kashiwanoha, Kashiwa, Chiba 2778581, Japan
关键词
spin crossover; Fe(III) complex; qsal ligand; thermal hysteresis; structure phase transition; counter-anion; solvate; lattice energy; optical conductivity spectrum; SCHIFF-BASE LIGANDS; IRON(III) COMPLEXES; MAGNETIC-PROPERTIES; QUINOLYLSALICYLALDIMINE COMPLEX; ELECTRICAL-CONDUCTIVITY; HALOGEN SUBSTITUTION; THERMAL HYSTERESIS; SOLVENT; BEHAVIOR;
D O I
10.3390/cryst9020081
中图分类号
O7 [晶体学];
学科分类号
0702 ; 070205 ; 0703 ; 080501 ;
摘要
New Fe(III) compounds from qsal ligand, [Fe(qsal)(2)](CH3OSO3) (1) and [Fe(qsal)(2)](CH3SO3)center dot 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 pi-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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页数:22
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