4 research outputs found

    Shell Model force field for Lead Zirconate Titanate Pb(Zr<sub>1–<i>x</i></sub>Ti<sub><i>x</i></sub>)O<sub>3</sub>

    No full text
    We have developed a shell model force field that reproduces the details of the phase diagram of the Pb­(Zr<sub>1–<i>x</i></sub> Ti<sub><i>x</i></sub>)­O<sub>3</sub>(PZT) solid solution compound, including the low- and high-temperature phases of PbZrO<sub>3</sub> and PbTiO<sub>3</sub>. The developed force field supports the temperature-induced phase transitions from cubic to low symmetry phases over the whole composition range and additionally reproduces the composition driven phase transitions. Indeed, the increase of Ti content induces a phase change of PZT from rhombohedral to tetragonal symmetry, mediated by a monoclinic phase, all in excellent agreement with the experiments

    A Polar Corundum Oxide Displaying Weak Ferromagnetism at Room Temperature

    No full text
    Combining long-range magnetic order with polarity in the same structure is a prerequisite for the design of (magnetoelectric) multiferroic materials. There are now several demonstrated strategies to achieve this goal, but retaining magnetic order above room temperature remains a difficult target. Iron oxides in the +3 oxidation state have high magnetic ordering temperatures due to the size of the coupled moments. Here we prepare and characterize ScFeO<sub>3</sub> (SFO), which under pressure and in strain-stabilized thin films adopts a polar variant of the corundum structure, one of the archetypal binary oxide structures. Polar corundum ScFeO<sub>3</sub> has a weak ferromagnetic ground state below 356 Kî—¸this is in contrast to the purely antiferromagnetic ground state adopted by the well-studied ferroelectric BiFeO<sub>3</sub>

    A Polar Corundum Oxide Displaying Weak Ferromagnetism at Room Temperature

    No full text
    Combining long-range magnetic order with polarity in the same structure is a prerequisite for the design of (magnetoelectric) multiferroic materials. There are now several demonstrated strategies to achieve this goal, but retaining magnetic order above room temperature remains a difficult target. Iron oxides in the +3 oxidation state have high magnetic ordering temperatures due to the size of the coupled moments. Here we prepare and characterize ScFeO<sub>3</sub> (SFO), which under pressure and in strain-stabilized thin films adopts a polar variant of the corundum structure, one of the archetypal binary oxide structures. Polar corundum ScFeO<sub>3</sub> has a weak ferromagnetic ground state below 356 Kî—¸this is in contrast to the purely antiferromagnetic ground state adopted by the well-studied ferroelectric BiFeO<sub>3</sub>

    A Polar Corundum Oxide Displaying Weak Ferromagnetism at Room Temperature

    No full text
    Combining long-range magnetic order with polarity in the same structure is a prerequisite for the design of (magnetoelectric) multiferroic materials. There are now several demonstrated strategies to achieve this goal, but retaining magnetic order above room temperature remains a difficult target. Iron oxides in the +3 oxidation state have high magnetic ordering temperatures due to the size of the coupled moments. Here we prepare and characterize ScFeO<sub>3</sub> (SFO), which under pressure and in strain-stabilized thin films adopts a polar variant of the corundum structure, one of the archetypal binary oxide structures. Polar corundum ScFeO<sub>3</sub> has a weak ferromagnetic ground state below 356 Kî—¸this is in contrast to the purely antiferromagnetic ground state adopted by the well-studied ferroelectric BiFeO<sub>3</sub>
    corecore