Spin-current interaction with a monodomain magnetic body: A model study

By Jonathan Z. Sun. 2000

942 citations recorded by the source corpus.

Subfields: Atomic and Molecular Physics, and Optics, Biomedical Engineering, Condensed Matter Physics

View Paper: https://www.semanticscholar.org/paper/aa5159e678a52edc3a43604a31e4b7afdba9f136

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In Atomic and Molecular Physics, and Optics

In Biomedical Engineering

In Condensed Matter Physics

Citations in the corpus

The emergence of spin electronics in data storage. (2007, background): “However, MRAM has other advantages such as potentially infinite endurance (against ~10(5) cycles for a Flash) and potential for sub-ns operation [66, 73, 74], that makes it competitive as “universal” memory.”
Spintronics: Fundamentals and applications (2004, neutral): “…has since been extensively studied both theoretically and experimentally (Bazaliy et al., 1998; Myers et al., 1999; Stiles and Zangwill, 2002; Sun, 2000; Tsoi et al., 1998; Waintal et al., 2000) and current-induced magnetization reversal was demonstrated at room temperature (Katine et al.,…”
Spintronics (2015, methodology): “The dynamic behavior can be studied through a modified Landau-LifshitzGilbert equation describing the damped precession of magnetization in the presence of STT and thermal excitation [Sun 2000].”
Perpendicular magnetic anisotropy at transition metal/oxide interfaces and applications (2017, methodology): “The critical current for STT-induced reversal of magnetization in the storage layer based on the LLG equation in the out-of-plane configuration is given by (Sun, 2000)”
Microwave oscillations of a nanomagnet driven by a spin-polarized current (2003, methodology): “To understand what type of motion may be associated with the different dynamical modes, we have computed solutions of the Landau–Lifshitz–Gilbert equation of motion for a single-domain magne”
Ultra-Fast Perpendicular Spin–Orbit Torque MRAM (2015, background): “This scaling is reminiscent of early spintransfer torque predictions [30] and experiments [31] where the injected spin current polarization is aligned along the uniaxial anisotropy axis.”
Current-induced spin-orbit torques in ferromagnetic and antiferromagnetic systems (2018, background): “…this case, the threshold current has the same form as that of the conventional STT switching for free and fixed layers with in-plane magnetization (Sun, 2000), and is given by (Lee et al., 2013) jsw,|| = α 2e ~ MstF ξjDL ( Bk,|| + Bd 2 ) , (62) where Bk,|| is the in-plane anisotropy field and Bd…”