TY - JOUR
T1 - Electronic properties in a five-coordinate azido complex of nonplanar iron(III) porphyrin
T2 - Revisiting to quantum mechanical spin admixing
AU - Neya, Saburo
AU - Takahashi, Akihiro
AU - Ode, Hirotaka
AU - Hoshino, Tyuji
AU - Ikezaki, Akira
AU - Ohgo, Yoshiki
AU - Takahashi, Masashi
AU - Furutani, Yuji
AU - Lórenz-Fonfría, Víctor A.
AU - Kandori, Hideki
AU - Hiramatsu, Hirotsugu
AU - Kitagawa, Teizo
AU - Teraoka, Junji
AU - Funasaki, Noriaki
AU - Nakamura, Mikio
PY - 2008
Y1 - 2008
N2 - The iron(III) azido complex of 5,10,15,20-tetraisopropylporphyrin was characterized with NMR, EPR, Mössbauer, and magnetic susceptibility. These physical methods indicate mixing of the high (S = 5/2) and intermediate (S = 3/2) spin-states of the iron atom. The results were interpreted in terms of the core contraction after nonplanar deformation of porphyrin ring by the bulky isopropyl substituents. In the IR spectrum of this complex, there are two signals at 2062 and 2048 cm-1 due to the antisymmetric vibration of the coordinated azido ligand. The split IR bands demonstrate that the two spin isomers are present, and that the S = 5/2 and 3/2 transition occurs sufficiently slow on the IR timeseale. This is in remarkable contrast with the homogeneous spin-mixing model proposed for the S = 5/2 and 3/2 system. The present observations further suggests that the three S = 5/2, 3/2, and 1 /2 states in iron(III) porphyrin commonly mix through thermal spin equilibrium.
AB - The iron(III) azido complex of 5,10,15,20-tetraisopropylporphyrin was characterized with NMR, EPR, Mössbauer, and magnetic susceptibility. These physical methods indicate mixing of the high (S = 5/2) and intermediate (S = 3/2) spin-states of the iron atom. The results were interpreted in terms of the core contraction after nonplanar deformation of porphyrin ring by the bulky isopropyl substituents. In the IR spectrum of this complex, there are two signals at 2062 and 2048 cm-1 due to the antisymmetric vibration of the coordinated azido ligand. The split IR bands demonstrate that the two spin isomers are present, and that the S = 5/2 and 3/2 transition occurs sufficiently slow on the IR timeseale. This is in remarkable contrast with the homogeneous spin-mixing model proposed for the S = 5/2 and 3/2 system. The present observations further suggests that the three S = 5/2, 3/2, and 1 /2 states in iron(III) porphyrin commonly mix through thermal spin equilibrium.
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U2 - 10.1246/bcsj.81.136
DO - 10.1246/bcsj.81.136
M3 - Article
AN - SCOPUS:57149086199
SN - 0009-2673
VL - 81
SP - 136
EP - 141
JO - Bulletin of the Chemical Society of Japan
JF - Bulletin of the Chemical Society of Japan
IS - 1
ER -