The electronic properties of copper oxides represent an historical challenge for first-principles calculations, since the low-magnetization state (S=1/2) of Cu2+ ions is not correctly described by standard theories (such as the local-spin density functional theory). Here we present results obtained through our novel self-interaction free density functional scheme (the pseudo-SIC [1]) for a range of different cuprates, with CuO2 units arranged in 3-dimensional (CuO doped with Mn), bidimensional (YBa 2Cu3O6+x), and one-dimensional (GeCuO 3.) fashion. In all the cases we give a sound description of the chemistry and the electronic and magnetic properties of these systems: In CuO Mn-doping acts as a single donor and induces a simultaneous insulating-to-metal and antiferromagnetic-to-ferromagnetic phase transition driven by double-exchange. In YBa2Cu3O6+x the phase transition from antiferromagnetic insulating to paramagnetic metal is mainly governed by the ordering of doping oxygens in the Cu(I)-O-Cu(I) chains. © 2008 IEEE.
Electronic properties and doping mechanism in cuprates by first-principles calculations
Filippetti, Alessio;Fiorentini, Vincenzo
2008-01-01
Abstract
The electronic properties of copper oxides represent an historical challenge for first-principles calculations, since the low-magnetization state (S=1/2) of Cu2+ ions is not correctly described by standard theories (such as the local-spin density functional theory). Here we present results obtained through our novel self-interaction free density functional scheme (the pseudo-SIC [1]) for a range of different cuprates, with CuO2 units arranged in 3-dimensional (CuO doped with Mn), bidimensional (YBa 2Cu3O6+x), and one-dimensional (GeCuO 3.) fashion. In all the cases we give a sound description of the chemistry and the electronic and magnetic properties of these systems: In CuO Mn-doping acts as a single donor and induces a simultaneous insulating-to-metal and antiferromagnetic-to-ferromagnetic phase transition driven by double-exchange. In YBa2Cu3O6+x the phase transition from antiferromagnetic insulating to paramagnetic metal is mainly governed by the ordering of doping oxygens in the Cu(I)-O-Cu(I) chains. © 2008 IEEE.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.