The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Feb. 28, 2023

Filed:

Apr. 16, 2020
Applicant:

University of Rochester, Rochester, NY (US);

Inventors:

Abdelrahman G. Qoutb, Rochester, NY (US);

Eby G. Friedman, Rochester, NY (US);

Assignee:

University of Rochester, Rochester, NY (US);

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
H01F 10/32 (2006.01); G11C 11/16 (2006.01); H03K 19/18 (2006.01); H01L 43/10 (2006.01); H01L 43/00 (2006.01); G11C 11/18 (2006.01); H01L 43/06 (2006.01); H01L 43/04 (2006.01);
U.S. Cl.
CPC ...
H01F 10/3286 (2013.01); G11C 11/161 (2013.01); G11C 11/1675 (2013.01); G11C 11/18 (2013.01); H01F 10/329 (2013.01); H01L 43/00 (2013.01); H01L 43/04 (2013.01); H01L 43/06 (2013.01); H01L 43/065 (2013.01); H01L 43/10 (2013.01); H03K 19/18 (2013.01); Y10S 148/109 (2013.01);
Abstract

A base element for switching a magnetization state of a nanomagnet includes a heavy-metal nanostrip having a surface. The heavy-metal nanostrip includes at least a first layer including a heavy metal and a second layer which includes a different heavy-metal. A ferromagnetic nanomagnet is disposed adjacent to the surface. The ferromagnetic nanomagnet includes a shape having a long axis and a short axis, the ferromagnetic nanomagnet having both a perpendicular-to-the-plane anisotropy Hand an in-plane anisotropy Hand the ferromagnetic nanomagnet having a first magnetization equilibrium state and a second magnetization equilibrium state. The first magnetization equilibrium state or the second magnetization equilibrium state is settable by a flow of electrical charge through the heavy-metal nanostrip. A direction of the flow of electrical charge through the heavy-metal nanostrip includes an angle ξ with respect to the short axis of the nanomagnet.


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