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Integration of Paramagnetic Diruthenium Complexes into an Extended Chain by Heterometallic Metal-Metal Bonds with Diplatinum Complexes.
Uemura, Kazuhiro; Uesugi, Naoyuki; Matsuyama, Akina; Ebihara, Masahiro; Yoshikawa, Hirofumi; Awaga, Kunio.
Affiliation
  • Uemura K; Department of Chemistry and Biomolecular Science, Faculty of Engineering, Gifu University , Yanagido 1-1, Gifu 501-1193, Japan.
  • Uesugi N; Department of Chemistry and Biomolecular Science, Faculty of Engineering, Gifu University , Yanagido 1-1, Gifu 501-1193, Japan.
  • Matsuyama A; Department of Chemistry and Biomolecular Science, Faculty of Engineering, Gifu University , Yanagido 1-1, Gifu 501-1193, Japan.
  • Ebihara M; Department of Chemistry and Biomolecular Science, Faculty of Engineering, Gifu University , Yanagido 1-1, Gifu 501-1193, Japan.
  • Yoshikawa H; Department of Chemistry and Research Center for Materials Science (RCMS), Nagoya University , Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan.
  • Awaga K; Department of Chemistry and Research Center for Materials Science (RCMS), Nagoya University , Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan.
Inorg Chem ; 55(14): 7003-11, 2016 Jul 18.
Article in En | MEDLINE | ID: mdl-27348516
ABSTRACT
We successfully obtained a paramagnetic one-dimensional (1D) chain complex [{Ru2(O2CCH3)4}{Pt2(piam)2(NH3)4}2]n(PF6)4n·4nH2O (2; piam = pivalamidate) extended by metal-metal bonds. Compound 2 comprises two types of metal species, ruthenium and platinum, where an acetate-bridged dinuclear ruthenium complex (i.e., [Ru2]) and a pivalamidate-bridged platinum complex (i.e., [Pt2]) are connected by axial metal-metal bonds, forming an attractive quasi-1D infinite chain that can be expressed as -{[Pt2]-[Ru2]-[Pt2]}n-. Such axial metal-metal bonds are attributed to the interaction between the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) along the z axis, where both the HOMO in [Pt2(II,II)] and the LUMO in [Ru2(II,II)] are σ* orbitals associated with metal cores. The crystal structure and X-ray photoelectron spectrum for 2 reveal that metal oxidation states are -{[Pt2(II,II)]-[Ru2(II,II)]-[Pt2(II,II)]}n-, where [Ru2(II,II)] can have an electronic configuration of σ(2)π(4)δ(2)δ*(2)π*(2) or σ(2)π(4)δ(2)π*(4). The magnetic susceptibility of 2 has a µeff [∝(χT)(1/2)] value of 2.77 µB per [Pt2(II,II)]-[Ru2(II,II)]-[Pt2(II,II)] unit at 300 K, showing that two unpaired electrons lie on π*(Ru2). Magnetic measurements performed at temperatures of 2-300 K indicate that S = 1 Ru2(II,II) units are weakly antiferromagnetically coupled (zJ = -1.4 cm(-1)) with a large zero-field splitting (D = 221 cm(-1)).

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Inorg Chem Year: 2016 Document type: Article Affiliation country: Japan

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Inorg Chem Year: 2016 Document type: Article Affiliation country: Japan