April 7 - 11, 2025
Seattle, Washington
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2025 MRS Spring Meeting & Exhibit
EL08.01.09

Experimental Confirmation of Predicted Cobalt-Based Magnetic Antiperovskite Nitrides

When and Where

Apr 7, 2025
11:15am - 11:30am
Summit, Level 4, Room 433

Presenter(s)

Co-Author(s)

Sita Dugu1,Sharad Mahatara1,Corlyn Regier2,Ian Leahy1,Andriy Zakutayev1,Jamie Neilson2,Sage Bauers1

National Renewable Energy Laboratory1,Colorado State University2

Abstract

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 X3AN (where X is a 3d metal Mn, Fe, Ni, Co) are subset of antiperovskite materials with exciting properties. Examples of magnetic antiperovskites include: Co3FeN, which has been reported as half-metallic, Fe3FeN (i.e., Fe4N) and its N-vacancy ordered derivative Fe16N2, which is the strongest known ferromagnet, and Mn3CuN, which exhibits a giant magnetostrictive effect. Recently, several Co-containing antiperovskites, including Co3PdN and Co3PtN 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 Co3PdN, Co3PtN, and Co3ZnN, fabricated via magnetron sputtering. Our findings show that Co3PdN and Co3ZnN exhibit greater stability compared to Co3PtN. Synchrotron X-ray diffraction data for stoichiometric Co3PdN and Co3ZnN reveal a cubic antiperovskite structure with lattice constants of 3.806 Å and 3.743 Å, respectively. Experimentally, Co3PdN 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, Co3ZnN undergoes a low-temperature transition near 40 K, accompanied by lower coercivity. Previous computational studies predicted a ferromagnetic ground state for Co3PdN, and we validate this by showing that the total energy of ferromagnetic Co3PdN is significantly lower than various antiferromagnetic configurations, by at least +88 meV/atom. Additionally, we present magnetotransport data collected from epitaxial Co3PdN films grown on SrTiO3 and MgO substrates. We compare Co3PdN to Co3PtN which, despite also being predicted as stable, does not adopt the antiperovskite structure.
This work provides the first experimental confirmation of the Co3PdN, Co3ZnN antiperovskite phase, highlighting its potential for further research into its magnetoelectric properties, as well as encouraging exploration of other Co3AN compounds waiting experimental realization.

Keywords

nitride | thin film

Symposium Organizers

Morgan Trassin, ETH Zurich
John Heron, University of Michigan
Dennis Meier, Norwegian University of Science and Technology
Michele Conroy, Imperial College London

Session Chairs

John Heron
Lynette Keeney

In this Session