Magnetic memory with chiral antiferromagnetic material for magnet switching
US-2019304525-A1 · Oct 3, 2019 · US
US10804459B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10804459-B2 |
| Application number | US-201816225071-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 19, 2018 |
| Priority date | Dec 19, 2018 |
| Publication date | Oct 13, 2020 |
| Grant date | Oct 13, 2020 |
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Spintronic devices based on metallic antiferromagnets having a non-collinear spin structure are provided. Also provided are methods for operating the devices. The spintronic devices are based on a bilayer structure that includes a spin torque layer of an antiferromagnetic material having a non-collinear triangular spin structure adjoining a layer of ferromagnetic material.
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What is claimed is: 1. A spintronic device comprising: a ferromagnetic layer comprising a ferromagnetic material having perpendicular magnetization; a spin-torque layer comprising a metallic antiferromagnetic material having a non-collinear spin structure adjoining the ferromagnetic layer at an interface, the metallic antiferromagnetic material characterized in that it is capable of generating spin currents having non-zero out-of-plane spin polarizations when an in-plane charge current is passed through the spin-torque layer; and a current source configured to pass an in-plane charge current through the spin torque layer. 2. The device of claim 1 , wherein the metallic antiferromagnetic material having a non-collinear spin structure comprises a nitride having the formula Mn 3 AN, where A is gallium, zinc, copper, or nickel. 3. The device of claim 2 , where A is gallium. 4. A method of modulating the magnetization in a spintronic device comprising: a ferromagnetic layer comprising a ferromagnetic material having a perpendicular magnetization; a spin-torque layer comprising a metallic antiferromagnetic material having a non-collinear spin structure in contact with the ferromagnetic layer at an interface; and a current source configured to pass an in-plane charge current through the spin-torque layer, the method comprising: passing an in-plane charge current through the spin-torque layer, whereby spin currents having out-of-plane spin polarizations are generated in the spin-torque layer giving rise to a spin torque in the ferromagnetic layer that modulates the magnetization of the ferromagnetic material. 5. The method of claim 4 , wherein the spin torque in the ferromagnetic layer switches the magnetization of the ferromagnetic material. 6. The method of claim 4 , wherein the metallic antiferromagnetic material having a non-collinear spin structure comprises a nitride having the formula Mn 3 AN, where A is gallium, zinc, copper, or nickel. 7. A magnetic tunnel junction device comprising; a magnetic tunnel junction comprising: a free magnetic layer comprising a ferromagnetic material having a perpendicular magnetization; a pinned layer comprising a ferromagnetic material having a fixed direction of magnetization; and a barrier layer comprising an electrically insulating material separating the ferromagnetic layer from the pinned layer; a spin torque layer comprising a metallic antiferromagnetic material having a non-collinear spin structure in contact with the free magnetic layer at an interface, the metallic antiferromagnetic material characterized in that it is capable of generating spin currents having non-zero out-of-plane spin polarizations when an in-plane charge current is passed through the spin-torque layer; a write current source configured to pass an in-plane charge current through the spin torque layer; a read current source configured to pass a charge current through the magnetic tunnel junction; and a voltage source configured to apply a bias voltage between the pinned layer and the spin-torque layer. 8. The device of claim 7 , wherein the metallic antiferromagnetic material having a non-collinear spin structure comprises a nitride having the formula Mn 3 AN, where A is gallium, zinc, copper, or nickel. 9. The device of claim 8 , where A is gallium. 10. A method of operating a magnetic tunnel junction device comprising: a magnetic tunnel junction comprising: a free magnetic layer comprising a ferromagnetic material having a perpendicular magnetization; a pinned layer comprising a ferromagnetic material having a fixed direction of magnetization; and a barrier layer comprising an electrically insulating material separating the ferromagnetic layer from the pinned layer; a spin torque layer comprising a metallic antiferromagnetic material having a non-collinear spin structure in contact with the free magnetic layer at an interface; a write current source configured to pass an in-plane charge current through the spin torque layer; and a read current source configured to pass a charge current through the magnetic tunnel junction, the method comprising: passing an in-plane write current through the spin torque layer, whereby spin currents having out-of-plane spin polarizations are generated in the spin-torque layer, giving rise to a spin torque in the free magnetic layer that switches the magnetization of the free magnetic layer; and passing a read current through the magnetic tunnel junction and measuring the resistance of the magnetic tunnel junction. 11. The method of claim 10 , wherein the metallic antiferromagnetic material having a non-collinear spin structure comprises a nitride having the formula Mn 3 AN, where A is gallium, zinc, copper, or nickel. 12. The method of claim 11 , where A is gallium. 13. The method of claim 6 , where A is gallium.
Spin-exchange coupled multilayers wherein the magnetisation of the free layer is switched by a spin-polarised current, e.g. spin torque effect · CPC title
Exchange coupling of magnetic films via an antiferromagnetic interface (H01F10/3268 takes precedence) · CPC title
Materials of the active region · CPC title
Constructional details · CPC title
Magnetoresistive devices · CPC title
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