Abstract
Bimetallic oxalates are molecule-based magnets with transition-metal ions M(II) and M′(III) arranged on an open honeycomb lattice. Performing a Holstein-Primakoff expansion, we obtain the spin-wave spectrum of antiferromagnetically coupled bimetallic oxalates as a function of the crystal-field angular momentum L2 and L3 on the M(II) and M′(III) sites. Our results are applied to the Fe(II)Mn(III), Ni(II)Mn(III) and V(II)V(III) bimetallic oxalates, where the spin-wave gap varies from 0 meV for quenched angular momentum to as high as 15meV. The presence or absence of magnetic compensation appears to have no effect on the spin-wave gap.
Original language | English |
---|---|
Article number | 016005 |
Journal | Journal of Physics Condensed Matter |
Volume | 21 |
Issue number | 1 |
DOIs | |
State | Published - 2009 |