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Second order anisotropy contribution in perpendicular magnetic tunnel junctions

2016/02/18 by A. A. Timopheev, Timopheev, A. A., R. Sousa +11 · 1 citation
Materials Science · Physics and Astronomy · #Anisotropy #Condensed matter physics #FOS: Physical sciences #Ferromagnetic resonance #Ferromagnetism #Geometry #Magnetic Properties and Applications #Magnetic anisotropy #Magnetic field #Magnetic properties of thin films #Magnetization #Magnetoresistance #Materials science #Mesoscale and Nanoscale Physics (cond-mat.mes-hall) #Optics #Perpendicular #Physics #Physics of Superconductivity and Magnetism #Tunnel magnetoresistance #cond-mat.mes-hall

paper · pdf · doi:10.48550/arxiv.1602.05815

published in arXiv (Cornell University) (Cornell University)

arxiv created 2016/02/18 · openalex publication_date 2016/02/18 · arxiv updated 2016/02/19 · openalex created_date 2019/06/27 · openalex updated_date 2026/08/04

Abstract

Magnetoresistance loops under in-plane applied field were measured on perpendicularly magnetized magnetic tunnel junction (pMTJ) pillars with nominal diameters ranging from 50 to 150 nm. By fitting the hard-axis magnetoresistance loops to an analytical model, the effective anisotropy fields in both free and reference layers were derived and their variations in temperature range between 340K and 5K were determined. It is found that an accurate fitting is possible only if a second-order anisotropy term of the form -K2cos4θ, is added to the fitting model. This higher order contribution exists both in the free and reference layers and its sign is opposite to that of the first order anisotropy constant, K1. At room temperatures the estimated -K2/K1 ratios are 0.1 and 0.24 for the free and reference layers, respectively. The ratio is more than doubled at low temperatures altering the ground state of the reference layer from 'easy-axis' to 'easy-cone' regime. Easy-cone state has clear signatures in the shape of the hard-axis magnetoresistance loops. The same behavior was observed in all measured devices regardless of their diameter. The existence of this higher order anisotropy was confirmed experimentally on FeCoB/MgO sheet films by ferromagnetic resonance technique. It is of interfacial nature and is believed to be linked to spatial fluctuations at the nanoscale of the anisotropy parameter at the FeCoB/MgO interface, in agreement with Dieny-Vedyayev model.

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