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:
Nov. 27, 2018

Filed:

Mar. 01, 2017
Applicant:

Riken, Saitama, JP;

Inventors:

Naoto Nagaosa, Tokyo, JP;

Wataru Koshibae, Saitama, JP;

Junichi Iwasaki, Tokyo, JP;

Masashi Kawasaki, Tokyo, JP;

Yoshinori Tokura, Tokyo, JP;

Yoshio Kaneko, Tokyo, JP;

Assignee:

RIKEN, Saitama, JP;

Attorney:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G11C 19/08 (2006.01); H01L 27/105 (2006.01); H01L 29/82 (2006.01); H01L 41/08 (2006.01); G11C 11/16 (2006.01);
U.S. Cl.
CPC ...
G11C 19/0866 (2013.01); G11C 11/1659 (2013.01); G11C 11/1673 (2013.01); G11C 11/1675 (2013.01); G11C 19/08 (2013.01); G11C 19/085 (2013.01); G11C 19/0808 (2013.01); G11C 19/0841 (2013.01); H01L 27/105 (2013.01); H01L 29/82 (2013.01); H01L 41/08 (2013.01);
Abstract

A magnetic element capable of generating and erasing a skyrmion, including a magnet shaped as a thin layer and including a structure surrounded by a nonmagnetic material; a current path provided surrounding an end region including an end portion of the magnet, on one surface of the magnet; and a skyrmion sensor that detects the generation and erasing of the skyrmion. With Wm being width of the magnet and hm being height of the magnet, a size of the magnet, with the skyrmion of a diameter λ being generated, is such that 2λ>Wm>λ/2 and 2λ>hm>λ/2. With W being width of the end region in a direction parallel to the end portion of the magnet and h being height of the end region in a direction perpendicular to the end portion of the magnet, the end region is such that λ≥W>λ/4 and 2λ>h>λ/2.


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