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BEOL compatible high tunnel magneto resistance perpendicular magnetic tunnel junctions using a sacrificial Mg layer as CoFeB free layer cap
46
Citations
11
References
2015
Year
Magnetic PropertiesFree Layer CapEngineeringMagnetic MaterialsMagnetoresistanceMagnetismMagnetic Data StorageNanoelectronicsMaterials ScienceMaterials EngineeringElectrical EngineeringMgo-based Tunnel JunctionsMagnetoresistive Random-access MemoryMicroelectronicsMagnetic MaterialSacrificial Mg LayerMagnetic MediumSpintronicsFerromagnetismNatural SciencesApplied PhysicsMagnetic PropertyMagnetic DeviceTa Deposition
Perpendicularly magnetized MgO-based tunnel junctions are envisaged for future generation spin-torque transfer magnetoresistive random access memory devices. Achieving a high tunnel magneto resistance and preserving it together with the perpendicular magnetic anisotropy during BEOL CMOS processing are key challenges to overcome. The industry standard technique to deposit the CoFeB/MgO/CoFeB tunnel junctions is physical vapor deposition. In this letter, we report on the use of an ultrathin Mg layer as free layer cap to protect the CoFeB free layer from sputtering induced damage during the Ta electrode deposition. When Ta is deposited directly on CoFeB, a fraction of the surface of the CoFeB is sputtered even when Ta is deposited with very low deposition rates. When depositing a thin Mg layer prior to Ta deposition, the sputtering of CoFeB is prevented. The ultra-thin Mg layer is sputtered completely after Ta deposition. Therefore, the Mg acts as a sacrificial layer that protects the CoFeB from sputter-induced damage during the Ta deposition. The Ta-capped CoFeB free layer using the sacrificial Mg interlayer has significantly better electrical and magnetic properties than the equivalent stack without protective layer. We demonstrate a tunnel magneto resistance increase up to 30% in bottom pinned magnetic tunnel junctions and tunnel magneto resistance values of 160% at resistance area product of 5 Ω.μm2. Moreover, the free layer maintains perpendicular magnetic anisotropy after 400 °C annealing.
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