Density functional analysis of the magnetic structure of Li3RuO4: importance of the Ru-O···O-Ru spin-exchange interactions and substitutional Ru defects at the Li sites.
暂无分享,去创建一个
W. Son | P. Manuel | D. Adroja | M. Whangbo
[1] A. Wibowo,et al. On the magnetic insulating states, spin frustration, and dominant spin exchange of the ordered double-perovskites Sr2CuOsO6 and Sr2NiOsO6: density functional analysis. , 2011, Inorganic chemistry.
[2] M. Whangbo,et al. On the high magnetic-ordering temperature of the 5d magnetic oxide Ca3LiOsO6 crystallizing in a trigonal crystal structure: density functional analysis. , 2011, Inorganic chemistry.
[3] M. Whangbo,et al. Finite magnetization plateau from a two-dimensional antiferromagnet: density functional analysis of the magnetic structure of Cu3(P2O6OH)2. , 2010, Inorganic chemistry.
[4] M. Whangbo,et al. Theoretical analysis of the spin exchange and magnetic dipole-dipole interactions leading to the magnetic structure of Ni3TeO6. , 2010, Inorganic chemistry.
[5] M. Whangbo,et al. Consequences of the intrachain dimer–monomer spin frustration and the interchain dimer–monomer spin exchange in the diamond-chain compound azurite Cu3(CO3)2(OH)2 , 2009, Journal of physics. Condensed matter : an Institute of Physics journal.
[6] K. Kakurai,et al. Magnetic Excitations of Spin-Gap System Na3Cu2SbO6 with Distorted Honeycomb Structure , 2008, 0806.4249.
[7] M. Whangbo,et al. Determination of the spin-lattice relevant for the quaternary magnetic oxide Bi4Cu3V2O14 on the basis of tight-binding and density functional calculations. , 2008, Inorganic chemistry.
[8] M. Whangbo,et al. Analysis of the spin lattice model for the spin-gapped layered compounds Na(3)Cu(2)SbO(6) and Na(2)Cu(2)TeO(6) on the basis of electronic structure calculations. , 2008, Inorganic chemistry.
[9] T. Saha‐Dasgupta,et al. Electronic structures and low-dimensional magnetic properties of the ordered rocksalt oxides Na 3 Cu 2 SbO 6 and Na 2 Cu 2 TeO 6 , 2007 .
[10] H. Xiang,et al. Absence of a spiral magnetic order inLi2CuO2containing one-dimensionalCuO2ribbon chains , 2007, 0708.1708.
[11] M. Soma,et al. Lithium Ruthenates : Controlling Dimensionality and Topology of Magnetic-Ion Arrangements(Cross-disciplinary physics and related areas of science and technology) , 2006, cond-mat/0611691.
[12] T. Kuwai,et al. Kikuchiet al.Reply , 2006 .
[13] Masatoshi Sato,et al. Spin-Gap Behavior of Na3Cu2SbO6 with Distorted Honeycomb Structure , 2006 .
[14] S Mitsudo,et al. Experimental observation of the 1/3 magnetization plateau in the diamond-chain compound Cu3(CO3)2(OH)2. , 2005, Physical review letters.
[15] A. Assoud,et al. Synthesis, structure, and magnetic properties of the layered copper(II) oxide Na2Cu2TeO6. , 2005, Inorganic chemistry.
[16] M. Whangbo,et al. Classical spin and quantum-mechanical descriptions of geometric spin frustration. , 2004, The Journal of chemical physics.
[17] K. Kosuge,et al. High-field ESR measurements of novel spin chain substance Bi4Cu3V2O14 , 2004 .
[18] Dadi Dai,et al. Spin exchange interactions and magnetic structures of extended magnetic solids with localized spins: theoretical descriptions on formal, quantitative and qualitative levels , 2003 .
[19] C. Grey,et al. Structural and magnetic properties of Li3RuO4 , 2003 .
[20] M. Kaburagi,et al. Magnetic properties of the S = 1/2 distorted diamond chain at T = 0 , 2003, cond-mat/0305057.
[21] H. Kikuchi,et al. Magnetic properties of the frustrated diamond chain compound Cu3(CO3)2(OH)2 , 2003 .
[22] C. Torardi,et al. Flux Growth of Vanadyl Pyrophosphate, (VO)2P2O7, and Spin Dimer Analysis of the Spin Exchange Interactions of (VO)2P2O7 and Vanadyl Hydrogen Phosphate, VO(HPO4)·0.5H2O , 2002 .
[23] G. Kido,et al. Antiferromagnetic Order in Bi4Cu3V2O14 with Novel Spin Chain , 2002 .
[24] M. Whangbo,et al. Spin-Hamiltonian and density functional theory descriptions of spin exchange interactions , 2001 .
[25] C. Humphreys,et al. Electron-energy-loss spectra and the structural stability of nickel oxide: An LSDA+U study , 1998 .
[26] S. Nagler,et al. Magnetic Excitations in the S=1/2 Alternating Chain Compound (VO)_2P_2O_7 , 1997, cond-mat/9704092.
[27] Burke,et al. Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.
[28] Kresse,et al. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. , 1996, Physical review. B, Condensed matter.
[29] G. Kresse,et al. Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set , 1996 .
[30] M. Whangbo,et al. Spin exchange interactions of a spin dimer: Analysis of broken-symmetry spin states in terms of the eigenstates of Heisenberg and Ising spin Hamiltonians , 2003 .
[31] John E. Greedan,et al. Geometrically frustrated magnetic materials , 2001 .