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Current-Induced Magnetization Switching in MgO Barrier Magnetic Tunnel Junctions With CoFeB-Based Synthetic Ferrimagnetic Free Layers

机译:具有基于CoFeB的合成亚铁磁自由层的MgO势垒磁性隧道结中的电流感应磁化开关

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We investigated the effect of using a synthetic ferrimagnetic (SyF) free layer in MgO-based magnetic tunnel junctions (MTJs) on current-induced magnetization switching (CIMS), particularly for application to spin-transfer torque random access memory (SPRAM). The employed SyF free layer had a Co$_{40}$Fe $_{40}$B$_{20}$ /Ru/Co$_{40}$Fe$_{40}$B $_{20}$and Co$_{20}$ Fe$_{60}$B$_{20}$/Ru/Co $_{20}$Fe$_{60}$ B$_{20}$structures, and the MTJs (100 $times$ (150–300) nm$^{2}$) were annealed at 300 $^{circ}$C. The use of SyF free layer resulted in low intrinsic critical current density $(J_{rm c0})$ without degrading the thermal-stability factor ($E/k_{rm B}T$, where $E, k_{rm B}$, and $T$ are the energy potential, the Boltzmann constant, and temperature, respectively). When the two CoFeB layers of a strongly antiferromagnetically coupled SyF free layer had the same thickness, $J_{rm c0}$ was reduced to $2hbox{–-}4 times 10^{6}$ A/cm$^{2}$ . This low $J_{rm c0}$ may be due to the decreased effective volume under the large spin accumulation at the CoFeB/Ru. The $E/k_{rm B}T$ was over 60, resulting in a retention time of over ten years and suppression of the write current dispersion for SPRAM. The use of the SyF free layer also resulted in a bistable (parallel/antiparallel) magnetization configuration at zero field, enabling the realization of CIMS without the need to apply external fields to compensate for the offset field.
机译:我们研究了在基于MgO的磁性隧道结(MTJ)中使用合成亚铁磁(SyF)自由层对电流感应磁化开关(CIMS)的影响,特别是应用于自旋转移矩随机存取存储器(SPRAM)。所使用的SyF自由层具有Co $ _ {40} $ Fe $ __ {40} $ B $ _ {20} $ / Ru / Co $ _ {40} $ Fe $ _ {40} $ B $ _ {20 } $和Co $ _ {{20} $ Fe $ _ {60} $ B $ _ {20} $ / Ru / Co $ _ {20} $ Fe $ _ {60} $ B $ _ {20} $结构, MTJs(100 $×$(150–300)nm $ ^ {2} $)在300 $ ^ {circ} $ C退火。 SyF自由层的使用导致较低的固有临界电流密度$(J_ {rm c0})$,而不会降低热稳定性因子($ E / k_ {rm B} T $,其中$ E,k_ {rm B} $和$ T $分别是势能,玻尔兹曼常数和温度。当强反铁磁耦合的SyF自由层的两个CoFeB层具有相同的厚度时,$ J_ {rm c0} $减小为$ 2hbox {-} 4倍10 ^ {6} $ A / cm $ ^ {2} $。较低的$ J_ {rm c0} $可能是由于在CoFeB / Ru处大量自旋积累下有效体积减小所致。 $ E / k_ {rm B} T $超过60,导致保留时间超过十年,并抑制了SPRAM的写入电流分散。 SyF自由层的使用还导致了零磁场下的双稳态(平行/反平行)磁化配置,从而无需使用外部磁场来补偿偏移磁场即可实现CIMS。

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