2016
DOI: 10.1016/j.cap.2016.09.004
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Spin-transfer-torque-induced zero-field microwave oscillator using a magnetic easy cone state

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Cited by 10 publications
(6 citation statements)
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“…This restriction is intrinsically valid for weak K 2 case for any value of the H x . In contrast, it fails for very small H x (<1 mT, planar saturation field ∼300 mT) and small voltages in the case for the strong K 2 since there is no any static equilibrium in such condition as previously reported by Jang et al [43] for H x = 0. Using (7) and (8) we can express this condition in the limit H x → 0:…”
Section: Analytical Solution For In-plane Field Configurationsupporting
confidence: 60%
See 3 more Smart Citations
“…This restriction is intrinsically valid for weak K 2 case for any value of the H x . In contrast, it fails for very small H x (<1 mT, planar saturation field ∼300 mT) and small voltages in the case for the strong K 2 since there is no any static equilibrium in such condition as previously reported by Jang et al [43] for H x = 0. Using (7) and (8) we can express this condition in the limit H x → 0:…”
Section: Analytical Solution For In-plane Field Configurationsupporting
confidence: 60%
“…One might note that the above case a) corresponds to the situation of the existence of an easy-cone state as recently reported in Ref. [43] while the case b) is the common perpendicular state ("up" or "down"). The relations given by Eqs.…”
Section: Analytical Solution For In-plane Field Configurationmentioning
confidence: 61%
See 2 more Smart Citations
“…Subsequently, several experimental studies focused on either this structure, putting in evidence the second order magnetic anisotropy for pMTJs with thin CoFeB layers (1.2-1.35 nm) using FMR, or magnetoresistance for patterned structures. [12][13][14] Other studies explored the influence of this effect on pMTJ state diagrams. [15][16][17][18][19] Reference 19 considered the influence of a second order anisotropy on the switching current.…”
mentioning
confidence: 99%