2012
DOI: 10.1143/apex.5.093008
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High Spin Torque Efficiency of Magnetic Tunnel Junctions with MgO/CoFeB/MgO Free Layer

Abstract: We present the results of a perpendicular magnetic tunnel junction (MTJ) that displays simultaneously low critical switching current and voltage, as well as high thermal stability factor. These results were achieved using a free layer of the MgO/CoFeB/MgO structure by increasing the spin torque efficiency to an average of 3.0 kBT/µA for 37-nm-diameter junctions, about three times that of a MgO/CoFeB/Ta free layer, which makes it the highest value reported to date. By comparing two films with different RA, henc… Show more

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Cited by 84 publications
(35 citation statements)
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“…The angular-momentum flow associated with the spin-polarized current from the first layer (commonly referred to as spin filtering) can be absorbed by the second ferromagnetic layer, thereby applying a spin transfer torque which can excite and even reverse its magnetization. When optimized, with nanosize contacts, these structures have magnetization switching current densities on the order of 10 10 A/m 2 giving switching currents of less than 50 μA, significantly more efficient than magnetic switching driven by a magnetic field due to a nearby current flow (often referred to as an “Oersted field”) [Jan et al ., 2012; Gajek et al ., 2012; Sato et al ., 2014]. Spin torque from a spin-polarized current can also be used to generate large-angle steady-state magnetic precession to create magnetic nano-oscillators, potentially useful for frequency-tunable microwave sources and detectors [Kiselev et al ., 2003; Silva and Rippard, 2008], to be discussed in Sec.…”
Section: Spin Transport At and Through Interfacesmentioning
confidence: 99%
“…The angular-momentum flow associated with the spin-polarized current from the first layer (commonly referred to as spin filtering) can be absorbed by the second ferromagnetic layer, thereby applying a spin transfer torque which can excite and even reverse its magnetization. When optimized, with nanosize contacts, these structures have magnetization switching current densities on the order of 10 10 A/m 2 giving switching currents of less than 50 μA, significantly more efficient than magnetic switching driven by a magnetic field due to a nearby current flow (often referred to as an “Oersted field”) [Jan et al ., 2012; Gajek et al ., 2012; Sato et al ., 2014]. Spin torque from a spin-polarized current can also be used to generate large-angle steady-state magnetic precession to create magnetic nano-oscillators, potentially useful for frequency-tunable microwave sources and detectors [Kiselev et al ., 2003; Silva and Rippard, 2008], to be discussed in Sec.…”
Section: Spin Transport At and Through Interfacesmentioning
confidence: 99%
“…It was recognized early that a free layer with perpendicular magnetic anisotropy (PMA) would greatly reduce the switching voltage, compared to an in-plane magnetic free layer with the same thermal stability [Slonczewski 1997, Sun 2000]. Recent rapid progress in the STT-RAM field is largely driven by breakthroughs in PMA materials [Kishi 2008, Ikeda 2010, Worledge 2011, Jan 2012. Most previous publications focused on the optimization of the free layer material, being CoFeB-based or L1 0 -based.…”
Section: Introductionmentioning
confidence: 99%
“…First principal calculations and many experiments [17] have proven that hybridization of Fe 3d and O 2p orbitals at the Fe\MgO interface will create a PMA in Fe. Other experiments proved that the dual layers of MgO in a MgO\CoFeB\MgO trilayer stack [1819] could also create a PMA in CoFeB. Furthermore, Dieny [15] showed that many different oxides can also give rise to an interfacial PMA.…”
Section: Discussionmentioning
confidence: 99%