Structural, electronic, and magnetic properties of Co4N thin films deposited using HiPIMS

We studied the growth behavior, structural, electronic, and magnetic properties of cobalt nitride (Co-N) thin films deposited using direct current (dc) and high power impulse magnetron sputtering (HiPIMS) processes. The N-2 partial gas flow (RN2) was varied in close intervals to achieve the optimum conditions for the growth of the tetra cobalt nitride (Co4N) phase. We found that Co-N films grown using the HiPIMS process adopt (111) orientation as compared to the growth taking place along the (100) direction in the dcMS process. It was observed that HiPIMS grown Co-N films were superior in terms of crystallite size and uniform surface morphology. The local structure of films was investigated using x-ray absorption fine structure (XAFS) measurements. We found that the high energy of adatoms in the HiPIMS technique assisted in the more excellent stabilization of fcc-Co and the novel Co4N phase relative to the dcMS process. Magnetic properties of Co-N thin films were studied using magneto-optical Kerr effect, vibrating sample magnetometry and polarized neutron reflectivity. It was found that though the saturation magnetization remains almost similar in films grown by dcMS or HiPIMS processes, they differ in terms of their magnetic anisotropy. Such variation can be understood in terms of differences in the growth mechanisms in dcMS and HiPIMS processes affecting the resulting Co4N phase's local structure. (C) 2020 Elsevier B.V. All rights reserved.

Automated summary

The growth behavior, structural, electronic, and magnetic properties of Co-N thin films deposited using direct current (dc) and high power impulse magnetron sputtering (HiPIMS) processes were studied. The HiPIMS process resulted in superior crystallite size, surface morphology, and stabilization of fcc-Co and Co4N phase compared to the dcMS process. Although films grown by dcMS or HiPIMS processes showed similar saturation magnetization, they differed in terms of magnetic anisotropy due to variations in the growth mechanisms affecting the local structure of the Co4N phase.