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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
来源:
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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