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Cation Ordering and Electron Transfer (Paperback, Softcover reprint of the original 1st ed. 1985): C Gleitzer, J.B Goodenough,... Cation Ordering and Electron Transfer (Paperback, Softcover reprint of the original 1st ed. 1985)
C Gleitzer, J.B Goodenough, B.G. Hyde, M. O'Keeffe, U Weser
R2,928 Discovery Miles 29 280 Ships in 10 - 15 working days
Structure and Bonding (Paperback, Softcover reprint of the original 1st ed. 1980): J.D. Dunitz, J.B Goodenough, Peter... Structure and Bonding (Paperback, Softcover reprint of the original 1st ed. 1980)
J.D. Dunitz, J.B Goodenough, Peter Hemmerich, J.A. Ibers, C.K. Jorgensen, …
R2,922 Discovery Miles 29 220 Ships in 10 - 15 working days
Localized to Itinerant Electronic Transition in Perovskite Oxides (Paperback, Softcover reprint of the original 1st ed. 2001):... Localized to Itinerant Electronic Transition in Perovskite Oxides (Paperback, Softcover reprint of the original 1st ed. 2001)
S.L. Cooper; Edited by John B. Goodenough; Contributions by T. Egami, J.B Goodenough, J.-S. Zhou
R8,559 Discovery Miles 85 590 Ships in 10 - 15 working days

Interest in the transition metal oxides with perovskite related structures goes back to the 1950s when the sodium tungsten bronzes NaxWO3 were shown to be metallic [1 ], the system Lal_xSr~MnO3 was found to contain a ferromagnetic conductive phase [2], and La0.sSr0.sCoO3 was reported to be a ferromagnetic metal, but with a peculiar magnetization of 1.5 #a/Co atom [3]. Stoichiometric oxide perovskites have the generic formula AMO3 in which the A site is at the center of a simple cubic array of M sites; the oxide ions form (180 4)) M O M bridges to give an MO3 array of corner shared MO6/2 octahedra and the larger A cations have twelvefold oxygen coordination. Mismatch between the A O and M O equilibrium bond lengths introduces internal stresses. A compressive stress on the MO3 array is accommodated by a lowering of the M O M bond angle from 180 to (180 4)); a tensile stress on the M O M bonds is accommodated by the formation of hexagonal polytypes [4].

Localized to Itinerant Electronic Transition in Perovskite Oxides (Hardcover, 2001 ed.): S.L. Cooper Localized to Itinerant Electronic Transition in Perovskite Oxides (Hardcover, 2001 ed.)
S.L. Cooper; Edited by John B. Goodenough; Contributions by T. Egami, J.B Goodenough, J.-S. Zhou
R8,717 Discovery Miles 87 170 Ships in 10 - 15 working days

Interest in the transition metal oxides with perovskite related structures goes back to the 1950s when the sodium tungsten bronzes NaxWO3 were shown to be metallic [1 ], the system Lal_xSr~MnO3 was found to contain a ferromagnetic conductive phase [2], and La0.sSr0.sCoO3 was reported to be a ferromagnetic metal, but with a peculiar magnetization of 1.5 #a/Co atom [3]. Stoichiometric oxide perovskites have the generic formula AMO3 in which the A site is at the center of a simple cubic array of M sites; the oxide ions form (180 4)) M O M bridges to give an MO3 array of corner shared MO6/2 octahedra and the larger A cations have twelvefold oxygen coordination. Mismatch between the A O and M O equilibrium bond lengths introduces internal stresses. A compressive stress on the MO3 array is accommodated by a lowering of the M O M bond angle from 180 to (180 4)); a tensile stress on the M O M bonds is accommodated by the formation of hexagonal polytypes [4].

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