The electronic and magnetic properties of the hexanuclear ferric wheel [ LiFe6(OCH3)12-(dbm)6] PF6 have been studied with all-electron Hartree-Fock and full-potential density functional calculations. The best agreement for the magnetic exchange coupling is at the level of the B3LYP hybrid functional. Surprisingly, the Hartree-Fock approximation gives the wrong sign for the exchange coupling. The local density approximation and the gradient corrected functional PBE strongly overestimate the exchange coupling due to the too large delocalization of the d-orbitals. These findings are supported by results from the Mulliken population analysis for the magnetic moments and the charge on the individual atoms
The magnetic interactions between rare-earth and Fe ions in hexagonal rare-earth ferrites (h-RFeO3),...
The electronic structure of strontium ferrite Sr3Fe2O6 was calculated using the tight-binding linear...
The hybrid B3PW91 exchange-correlation functional is used to calculate hyperfine fields at lanthanid...
We present an ab initio study of electronic correlation effects in a molecular cluster derived from ...
The Li-centered 'ferric wheel' molecules with six oxo-bridged iron atoms form molecular crystals. We...
The electronic structure of strontium ferrite Sr 3Fe 2O 6 was calculated using the tight-binding lin...
The orbital magnetic moment and related phenomena in the 3d and 5f electron systems are examined by ...
Controlling spin Hamiltonian parameters such as magnetic exchange and magnetic anisotropy of polynuc...
The calculation of interatomic magnetic exchange interactions entering the Heisenberg model is outli...
The magnetic and electronic structure of strontium hexaferrite SrFe12O19 has been investigated using...
After a general introduction into the field of molecular magnets the discussion focuses on a more s...
A series of electric and magnetic properties of hexafluorobenzene have been calculated, including t...
FeGe in the B20 phase is an experimentally well-studied prototypical chiral magnet exhibiting helica...
The ability of different density functionals to describe the structural and energy differences betwe...
(formula presented) is one of the most puzzling compounds among transition metal oxides because of i...
The magnetic interactions between rare-earth and Fe ions in hexagonal rare-earth ferrites (h-RFeO3),...
The electronic structure of strontium ferrite Sr3Fe2O6 was calculated using the tight-binding linear...
The hybrid B3PW91 exchange-correlation functional is used to calculate hyperfine fields at lanthanid...
We present an ab initio study of electronic correlation effects in a molecular cluster derived from ...
The Li-centered 'ferric wheel' molecules with six oxo-bridged iron atoms form molecular crystals. We...
The electronic structure of strontium ferrite Sr 3Fe 2O 6 was calculated using the tight-binding lin...
The orbital magnetic moment and related phenomena in the 3d and 5f electron systems are examined by ...
Controlling spin Hamiltonian parameters such as magnetic exchange and magnetic anisotropy of polynuc...
The calculation of interatomic magnetic exchange interactions entering the Heisenberg model is outli...
The magnetic and electronic structure of strontium hexaferrite SrFe12O19 has been investigated using...
After a general introduction into the field of molecular magnets the discussion focuses on a more s...
A series of electric and magnetic properties of hexafluorobenzene have been calculated, including t...
FeGe in the B20 phase is an experimentally well-studied prototypical chiral magnet exhibiting helica...
The ability of different density functionals to describe the structural and energy differences betwe...
(formula presented) is one of the most puzzling compounds among transition metal oxides because of i...
The magnetic interactions between rare-earth and Fe ions in hexagonal rare-earth ferrites (h-RFeO3),...
The electronic structure of strontium ferrite Sr3Fe2O6 was calculated using the tight-binding linear...
The hybrid B3PW91 exchange-correlation functional is used to calculate hyperfine fields at lanthanid...