23.
    发明专利
    未知

    公开(公告)号:DE60113136T2

    公开(公告)日:2006-03-30

    申请号:DE60113136

    申请日:2001-09-26

    Applicant: IBM

    Abstract: A ferromagnetic pinned layer (1) kept at a fixed magnetic orientation by a pinning layer (4) is separated from a ferromagnetic free layer (3) by a Mott insulator coupling layer (2). A controllable voltage source (5) is connected between the pinned layer (1) and the free layer (3). A sublayer of the coupling layer (2) whose width (d) increases with the voltage is converted to an electrically conducting and magnetically coupling metallic state. The magnetic exchange field acting on the free layer (3) which is controlled by the applied voltage via the width (d) of the electrically conducting sublayer of the coupling layer (2) can be used to switch the free layer (3) between states of parallel and antiparallel orientations with respect to the magnetic orientation of the pinned layer (1). This is used in memory cells and in a write head.

    25.
    发明专利
    未知

    公开(公告)号:DE69319933D1

    公开(公告)日:1998-08-27

    申请号:DE69319933

    申请日:1993-11-03

    Applicant: IBM

    Abstract: PCT No. PCT/EP93/03079 Sec. 371 Date May 2, 1996 Sec. 102(e) Date May 2, 1996 PCT Filed Nov. 3, 1993 PCT Pub. No. WO95/12882 PCT Pub. Date May 11, 1995An apparatus and a method for retrieving data stored on a magnetic medium with a high resolution is described. It is characterized by measuring a tunneling current which is partly depending on the magnetization of the medium (1). This dependence is caused by irradiating the medium (1) with polarized non-ionizing light. The tunneling current can be measured with a high lateral resolution by applying a probing tip (2) as known from conventional scanning tunneling microscopy or related techniques.

    Ferromagnetic device providing high domain wall velocities

    公开(公告)号:GB2500832B

    公开(公告)日:2015-12-09

    申请号:GB201310338

    申请日:2012-02-03

    Applicant: IBM

    Abstract: The invention is directed to a method of manufacturing a ferromagnetic device (10), having an elongated structure extending along a longitudinal direction (11), comprising a ferromagnetic material, wherein a transverse cross section (20) of the ferromagnetic material, perpendicular to said longitudinal direction, is designed to provide a domain wall velocity above the Walker breakdown limit of the ferromagnetic material. In particular, at least a portion (21-23) of a peripheral contour of the ferromagnetic material forms, in the transverse cross-section (20), a non-orthogonal convex set. For example, the whole peripheral contour may realize a (non-orthogonal) convex polygon.

    Ferromagnetic device providing high domain wall velocities

    公开(公告)号:GB2500832A

    公开(公告)日:2013-10-02

    申请号:GB201310338

    申请日:2012-02-03

    Applicant: IBM

    Abstract: The invention is directed to a ferromagnetic device (10), having an elongated structure extending along a longitudinal direction (11), comprising a ferromagnetic material, wherein a transverse cross section (20) of the ferromagnetic material, perpendicular to said longitudinal direction, is designed to provide a domain wall velocity above the Walker breakdown limit of the ferromagnetic material. In particular, at least a portion (21 - 23) of a peripheral contour of the ferromagnetic material forms, in the transverse cross-section (20), a non-orthogonal convex set. For example, the whole peripheral contour may realize a (non- orthogonal) convex polygon.

    Ferromagnetische Einheit, die hohe Domänenwandgeschwindigkeiten gewährleistet

    公开(公告)号:DE112012000271T5

    公开(公告)日:2013-09-19

    申请号:DE112012000271

    申请日:2012-02-03

    Applicant: IBM

    Abstract: Die Erfindung ist auf eine ferromagnetisches Einheit (10) mit einer länglichen Struktur, die sich entlang einer Längsrichtung (11) erstreckt, gerichtet, das einen ferromagnetischen Werkstoff aufweist, wobei ein transversaler Querschnitt (20) des ferromagnetischen Werkstoffs senkrecht zu der Längsrichtung so entworfen ist, dass er eine Domänenwand-Geschwindigkeit über der Walker-Durchbruchgrenze des ferromagnetischen Werkstoffs gewährleistet. Insbesondere bildet wenigstens ein Abschnitt (21 bis 23) einer peripheren Kontur des ferromagnetischen Werkstoffs in dem transversalen Querschnitt (20) einen nicht-orthogonalen konvexen Aufbau. Die gesamte periphere Kontur kann z. B. ein (nicht-orthogonales) konvexes Polygon bilden.

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