2021
DOI: 10.1063/5.0048926
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Field-free magnetization switching induced by the unconventional spin–orbit torque from WTe2

Abstract: Spin–orbit torque provides a highly efficient way to achieve current-induced magnetization switching, which relies on charge-to-spin conversion of the spin source layer. However, in the conventional heavy metal/ferromagnetic layer, the generated spin–orbit torque is limited to in-plane, which cannot deterministically switch the perpendicularly magnetized ferromagnets, and thus impedes practical application for high-density magnetic memory. In this work, deterministic switching of perpendicular magnetization is… Show more

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Cited by 41 publications
(23 citation statements)
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“…The chiral symmetry breaking by a gradient of magnetic anisotropy or saturation magnetization can also induce field-free switching 15 . Different from the above approaches that require asymmetric designs in device/film structures, recent works utilized the crystal symmetry to engineer the field-free switching in the WTe 2 /FM bilayer 16 18 and the CuPt/FM bilayer 19 . Although largely explored, the existing field-free switching in the above SOT bilayers/trilayers has some intrinsic disadvantages.…”
Section: Introductionmentioning
confidence: 99%
“…The chiral symmetry breaking by a gradient of magnetic anisotropy or saturation magnetization can also induce field-free switching 15 . Different from the above approaches that require asymmetric designs in device/film structures, recent works utilized the crystal symmetry to engineer the field-free switching in the WTe 2 /FM bilayer 16 18 and the CuPt/FM bilayer 19 . Although largely explored, the existing field-free switching in the above SOT bilayers/trilayers has some intrinsic disadvantages.…”
Section: Introductionmentioning
confidence: 99%
“…Development of high-density magnetic memory and computing technologies requires energy-efficient and scalable electrical switching of perpendicular magnetization. Microscopically, perpendicular magnetization can be switched by a current of transverse spins (σy) under the assist of an in-plane effective magnetic field along current (𝐻 𝑥 eff , to overcome the Dzyaloshinskii-Moriya interaction or to break the switching symmetry) 1 , or by an antidamping spin torque exerted by high-density current of perpendicular spins (σz) [2][3][4][5][6][7][8][9][10] , or by a strong perpendicular effective magnetic field (𝐻 𝑧 eff ) [11][12][13][14][15] . Since the first method (σy+𝐻 𝑥 eff ) is hardly energy-efficient or scalable, searching of σz or 𝐻 𝑧 eff in magnetic heterostructures becomes a very hot topic.…”
Section: Introductionmentioning
confidence: 99%
“…In this scenario, the spin electrons in the Pt layer with polarization along + p y (or − p y ) have been realigned, causing the spin polarization with an out-of-plane component. To confirm the existence and contribution of the out-of-plane spin-orbit torque contribution to the field-free SOT switching in the particular system, , we carried out the measurements with shifting V xy loops under different DC currents I DC . Figure a,b shows the V xy shift loops for MgO/Pt/Co samples at H x = 0 and H x = 520 Oe, respectively.…”
Section: Resultsmentioning
confidence: 99%