Apr 7, 2025
11:15am - 11:30am
Summit, Level 4, Room 433
Sita Dugu1,Sharad Mahatara1,Corlyn Regier2,Ian Leahy1,Andriy Zakutayev1,Jamie Neilson2,Sage Bauers1
National Renewable Energy Laboratory1,Colorado State University2
Nitrides of the form X
3AN (where X is a 3d metal Mn, Fe, Ni, Co) are subset of antiperovskite materials with exciting properties. Examples of magnetic antiperovskites include: Co
3FeN, which has been reported as half-metallic, Fe
3FeN (i.e., Fe
4N) and its N-vacancy ordered derivative Fe
16N
2, which is the strongest known ferromagnet, and Mn
3CuN, which exhibits a giant magnetostrictive effect. Recently, several Co-containing antiperovskites, including Co
3PdN and Co
3PtN were predicted to be stable, despite no experimental reports.
In this study, we investigate the synthesis, stability, and magnetic properties of cobalt-based thin films Co
3PdN, Co
3PtN, and Co
3ZnN, fabricated via magnetron sputtering. Our findings show that Co
3PdN and Co
3ZnN exhibit greater stability compared to Co
3PtN. Synchrotron X-ray diffraction data for stoichiometric Co
3PdN and Co
3ZnN reveal a cubic antiperovskite structure with lattice constants of 3.806 Å and 3.743 Å, respectively. Experimentally, Co
3PdN is identified as a soft magnetic material, with a low-temperature coercive field (
HC) of 200 Oe at 3 K. Stability assessments through high-temperature magnetometry and temperature-dependent X-ray diffraction reveal a Curie temperature (
TC) of approximately 600 K and a decomposition temperature around 700 K. In contrast, Co
3ZnN undergoes a low-temperature transition near 40 K, accompanied by lower coercivity. Previous computational studies predicted a ferromagnetic ground state for Co
3PdN, and we validate this by showing that the total energy of ferromagnetic Co
3PdN is significantly lower than various antiferromagnetic configurations, by at least +88 meV/atom. Additionally, we present magnetotransport data collected from epitaxial Co
3PdN films grown on SrTiO
3 and MgO substrates. We compare Co
3PdN to Co
3PtN which, despite also being predicted as stable, does not adopt the antiperovskite structure.
This work provides the first experimental confirmation of the Co
3PdN, Co
3ZnN antiperovskite phase, highlighting its potential for further research into its magnetoelectric properties, as well as encouraging exploration of other Co
3AN compounds waiting experimental realization.