Structure and magnetism of [n-BuNH3]12[Cu4(GeW9O34)2].14H2O sandwiching a rhomblike Cu4(8+) tetragon through alpha-Keggin linkage.
A sandwich-type polyoxometalate, [Cu(4)(GeW(9)O(34))(2)](12-) (1a), in which two B-alpha-[GeW(9)O(34)](12-) ligands sandwich a rhomblike Cu(4)(8+) tetragon through alpha-Kappaeggin linkage, is first isolated as a [n-BuNH(3)](+) salt, [n-BuNH(3)](12)[Cu(4)(GeW(9)O(34))(2)].14H(2)O (1). A Cu(4)O(14) cluster for the rhomblike Cu(4)(8+) tetragon in 1a with C(2h) local symmetry consists of two Jahn-Teller (JT) distorted CuO(6) octahedra (at internal sites) with a short diagonal Cu(int)...Cu(int) distance of 3.10-3.11 A and two CuO(5) square pyramids (at external site) with a long diagonal Cu(ext)...Cu(ext) distance of 5.34-5.35 A, the feature of which is different from [Cu(4)(H(2)O)(2)(GeW(9)O(34))(2)](12-) (2a), comprising the four JT-distorted CuO(6) octahedral Cu(4)(8+) tetragons through beta-Keggin linkage: the axial Cu(ext)-O bond distance (2.27-2.29 A) for 1a is shorter than the corresponding JT-axial distance (2.36 A) for 2a. Measurements of magnetic susceptibility, magnetization, and electron spin resonance spectroscopy for 1 are carried out for better understanding of the molecular magnetism of the Cu(4)(8+) tetragon in comparison with 2a. The analysis of the magnetic behavior, based on the isotropic Heisenberg spin Hamiltonian comprising three exchange parameters (J, J', and J''), gives J = -24.1 cm(-1) for the Cu(ext)..Cu(int) sides, J' = -99.1 cm(-1) for the Cu(int)...Cu(int) diagonal, and J'' = +0.04 cm(-1) for the Cu(ext)...Cu(ext) diagonal of the Cu(4)(8+) rhombus. The S = 1 ground state of 1 displays g(||) = 2.42, g( perpendicular)= 2.07, D = -1.44 x 10(-2) cm(-1), and |A(Cu||)| = 46.5 x 10(-4) cm(-1). An observation of the asymmetric magnetization between a positive and a negative pulsed field (up to 10(3) T/s) at 0.5 K on the hysteresis loop indicates the quantum tunneling at zero field. The magnetic exchange interactions of four unpaired d(x(2)-y(2))-electron spins are discussed in terms of the point-dipole approximation, and the primary contribution to D is implied to come from the magnetic dipole-dipole interaction between two spins at the Cu(ext) centers.
Yamase
Toshihiro
T
Chemical Resources Laboratory, Tokyo Institute of Technology, R1-21 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan. tyamase@res.titech.ac.jp
Abe
Hiroko
H
Ishikawa
Eri
E
Nojiri
Hiroyuki
H
Ohshima
Yuhgo
Y
D003300:Copper / Q000737:chemistry*; D018360:Crystallography, X-Ray; D004578:Electron Spin Resonance Spectroscopy; D004583:Electrons; D008280:Magnetics; D009942:Organometallic Compounds / Q000737:chemistry*; D010100:Oxygen / Q000737:chemistry; D013696:Temperature
C535051:(n-BuNH3)12(Cu4(GeW9O34)2); D009942:Organometallic Compounds; D003300:Copper; D010100:Oxygen