Handbook of Magnetism and Advanced Magnetic Materials 2007
DOI: 10.1002/9780470022184.hmm210
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Current Induced Domain‐wall Motion in Magnetic Nanowires

Abstract: Recent research on current‐induced domain‐wall motion in magnetic nanowires is reviewed. The first part of the article is devoted to theoretical models and micromagnetic simulations. We first describe the magnetic structure of head‐to‐head domain walls, and then discuss theories of their interaction with spin‐polarized current. The role of both adiabatic and nonadiabatic spin‐transfer torques is discussed in the framework of an analytical one‐dimensional model and micromagnetic simulations. The second part of … Show more

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Cited by 17 publications
(11 citation statements)
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References 171 publications
(268 reference statements)
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“…The dimensions of the notch structures were chosen to be comparable with the extent of the DW width using the definitions given in Ref. 13 so as to present an abrupt change to the potentialenergy landscapes. We present detailed results for nanowires nominally 300 nm wide with notch structures of nominal depth approximately 50% of the wire width, as shown in Fig.…”
Section: Methodsmentioning
confidence: 99%
“…The dimensions of the notch structures were chosen to be comparable with the extent of the DW width using the definitions given in Ref. 13 so as to present an abrupt change to the potentialenergy landscapes. We present detailed results for nanowires nominally 300 nm wide with notch structures of nominal depth approximately 50% of the wire width, as shown in Fig.…”
Section: Methodsmentioning
confidence: 99%
“…The domain wall internal structure depends on the thickness, width and material of the constituting magnetic nanostructure178. This internal structure has a strong influence on the DW dynamics, which is of uttermost importance for devices in which the domain wall position is controlled and manipulated by field910111213 or current pulses141516.…”
mentioning
confidence: 99%
“…Furthermore, since dm z /dx is no longer 0, the terms in the LLG equation (1) containing dm/dx gain additional character. The adiabatic STT term has the wellknown effect of propagating the domain walls [16], which in the case of bound domain walls means they merely shift along the nanowire. The nonadiabatic term has the more interesting effect of rotating the magnetization counterclockwise in the left domain wall and clockwise in the right one.…”
Section: Discussionmentioning
confidence: 99%