IP Library Granted Patent US 10,804,459
Granted Patent B2
US 10,804,459 · App. 16/225,071 · Granted Oct 13, 2020

Non-collinear antiferromagnets for high density and low power spintronics devices

Inventors: Chang-Beom Eom (Madison, WI); Tianxiang Nan (Madison, WI)
Assignee: WISCONSIN ALUMNI RESEARCH FOUNDATION
H01L43/10H01F10/002H01F10/12H01L43/04H01L43/06
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Quick Facts
Patent No.
US 10,804,459
App. No.
16/225,071
Granted
Oct 13, 2020
Kind
B2
Abstract

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.

Claims (37)

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.

Assignments (2)
CONFIRMATORY LICENSE Recorded Mar 26, 2020
From: UNIVERSITY OF WISCONSIN, MADISON
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 052249/0367 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 25, 2019
From: EOM, CHANG-BEOM; NAN, TIANXIANG
To: WISCONSIN ALUMNI RESEARCH FOUNDATION
Reel/Frame 048144/0467 →
Continuity (1)
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