序号 | 专利名 | 申请号 | 申请日 | 公开(公告)号 | 公开(公告)日 | 发明人 |
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101 | Magnetoresistive device and electronic device | US10228602 | 2002-08-27 | US20030042562A1 | 2003-03-06 | Carsten Giebeler; Kars-Michiel Hubert Lenssen; Stephan Johann Zilker; Reinder Coehoorn |
A magnetoresistive device (11) having a lateral structure and provided with a non-magnetic spacer layer (3) of organic semiconductor material allows the presence of an additional electrode (19). With this electrode (19), a switch-function is integrated into the device (11). Preferably, electrically conductive layers (13,23) are present for the protection of the ferromagnetic layers (1,2). The magnetoresistive device (11) is suitable for integration into an array so as to act as an MRAM device. | ||||||
102 | Magnetic multilayered films with reduced magnetostriction | US09894193 | 2001-06-27 | US20030002227A1 | 2003-01-02 | James Devereaux Jarratt |
It is the primary object of the present invention to provide a shield and pole material with reduced magnetostriction while preserving good magnetic characteristics. This material is used in recording heads in tape and disk drives. The material is a repeating sequence of three layers. One layer is FeX(N) where the (N) indicates a nitrogenated film and the additional element, X, is preferentially Ta but can be selected from a group of elements. Another layer is made from a NiFe alloy. The third layer, disposed between the FeX(N) and NiFe layers is tantalum. The sequence of three layers is repeated to build the required thickness for the final material. | ||||||
103 | Unidirectional gyrotropic photonic crystal and applications for the same | US10127649 | 2002-04-22 | US20020162988A1 | 2002-11-07 | Alexander Figotin; Ilya Vitebskiy |
An unidirectional gyrotropic photonic crystal allows electromagnetic wave propagation in a certain direction at a certain frequency and, at the same time, impedes electromagnetic wave propagation in the opposite direction. The electromagnetic wave with impeded propagation, called the nullfrozen modenull, ideally has zero group velocity and does not transfer the electromagnetic energy. A unidirectional gyrotropic photonic crystal is a periodic composite, incorporating a component displaying Faraday rotation. The property of unidirectionality can be achieved in gyrotropic photonic crystals by proper choices of constituents and their space arrangement. The invention can be used to enhance the capability and performance of microwave, millimeter wave, and submillimeter wave antennas, delay lines, nonlinear and nonreciprocal elements. It can also be used in integrated microwave circuitry. | ||||||
104 | Exchange coupling film, magnetoresistance effect device, magnetoresistance effective head and method for producing exchange coupling film | US09834716 | 2001-04-13 | US20020006529A1 | 2002-01-17 | Hiroshi Sakakima; Eiichi Hirota; Yasuhiro Kawawake; Mitsuo Satomi; Yasunari Sugita |
An exchange coupling film of the present invention includes a ferromagnetic layer and a pinning layer which is provided in contact with the ferromagnetic layer for pinning a magnetization direction of the ferromagnetic layer, the pinning layer including an (AB)2Ox layer, wherein: O denotes an oxygen atom; 2.8 | ||||||
105 | Magnetic field sensor and method for making same | US09341694 | 1999-07-26 | US06291993B1 | 2001-09-18 | Albert Fert; Frédéric Petroff; Luiz Fernando Schelp; Alain Schuhl |
A magnetic sensor having a layer of nonmagnetic insulator including at least one layer of ferromagnetic particles. This combination of layers is sandwiched between two ferromagnetic electrodes. Electrons are transported by the tunneling effect between each electrode and the ferromagnetic particles. The tunneling resistance depends on the orientation of the magnetization of the electrodes and therefore varies in the presence of the magnetic field. The multichannel and multistage nature of the tunneling conduction eliminates the problems of short-circuiting by porosity, thus leading to less difficult fabrication and improved robustness in terms of breakdown. The possible thermal fluctuations of the magnetic moments of the aggregates can be suppressed by the choice of a magnetic material for the part of the insulating layer which contains the aggregates. | ||||||
106 | Magnetic field responsive device having giant magnetoresistive material and method for forming the same | US750689 | 1997-04-07 | US5886523A | 1999-03-23 | Michael Richard John Gibbs; Gillian Anne Gehring; Harry Jarratt Blythe |
A magnetic field responsive device which includes: an electrically insulating substrate (2), a layer of an electrically conductive soft magnetic material (3), a layer of giant magneto-resitive (GMR) material (5) arranged in electrical contact with ethe layer of electrically conductive soft magnetic material, the thickness of the GMR material layer being not greater than twice the mean free path of an electron in the said GMR material, the layers being arranged in any order or position on the substrate and having opposed directions of mangetisation in zero magnectic field. | ||||||
107 | Magneto-optic compositionally modulated structure | US685741 | 1996-07-24 | US5858565A | 1999-01-12 | Randall H. Victora; Charles F. Brucker; Tukaram K. Hatwar |
A compositionally modulated magneto-optic structure includes a plurality of layers defining a layer stack, the overall layer stack including the elements Tb, Fe, and Pb; or the elements Tb, Co, and Pb; or the elements Tb, Fe, and Bi; or the elements Tb, Co and Bi. | ||||||
108 | Thin film composite having ferromagnetic and piezoelectric properties comprising a layer of Pb-Cd-Fe and a layer of Cr-Zn-(Te or Tl) | US779353 | 1997-01-06 | US5718983A | 1998-02-17 | Shimon Gendlin |
A composition of materials having ferromagnetic and piezoelectric properties is disclosed. In the preferred embodiment, the composition of materials comprises a first layer of Pb.sub.(1-x-y) Cd.sub.x Fe.sub.y and a second layer of Cr.sub.(1-z-w) Zn.sub.z Te.sub.w where x, y, z and w are values within the ranges of 0.38.ltoreq.x.ltoreq.0.042, 0.08.ltoreq.y.ltoreq.0.094, 0.38.ltoreq.z.ltoreq.0.41, 0.28.ltoreq.w.ltoreq.0.31, and 0.25.ltoreq.(1-z-w).ltoreq.0.32. Additionally, each of the layers contain the elements of Bi, O, and S. A random-accessible, non-volatile memory built using the This memory provides for storing two independent bits of binary information in a single storage cell. Each cell comprises two orthogonal address lines formed on the opposite surface of a Si substrate, a composition of materials of the present invention formed over each of the address lines, and an electrode formed over each composition of materials. The data is stored electromagnetically and retrieved as a piezoelectric voltage. | ||||||
109 | Multilayered sendust films with a gas-doped sendust seed layer | US594359 | 1996-01-30 | US5686193A | 1997-11-11 | John David Westwood |
A layered magnetic structure with a seed layer on a substrate and a bulk layer on the seed layer. The seed layer is a gas-doped sendust layer with a thickness of 100-800 .ANG.. The bulk layer is sendust with a thickness of 0.3-10.0 .mu.m. The seed layer and the bulk layer have different weight compositions. | ||||||
110 | Perpendicular magnetic film, multilayered film for perpendicular magnetic film and process for producing perpendicular magnetic film | US158854 | 1993-11-29 | US5496631A | 1996-03-05 | Kousaku Tamari |
Disclosed herein is a perpendicular magnetic film comprising a spinel thin film which is formed on a substrate, which contains Fe as the main ingredient and further contains Co and Ni, and which has a coercive force of less than 3000 Oe, the plane (400) thereof being predominantly oriented in parallel with said substrate, the spacing of the plane (400) being not more than 2.082 .ANG., the molar ratio of Co to Fe being 0.005 to 0.32 and the molar ratio of Ni to Co being at least 0.6. | ||||||
111 | Integrated common mode and differential mode inductor device | US968759 | 1992-10-30 | US5313176A | 1994-05-17 | Anand K. Upadhyay |
An integrated EMI/RFI Filter Magnetic has differential and common mode inductors wound about an I-Core. The I-Core is juxtaposed with an E-Core, with the end surfaces of the E-Core legs facing the I-Core. The magnetic has a substantially closed magnetic path for the differential inductors and the common mode inductors. | ||||||
112 | Magnetoresistance effect element | US824005 | 1992-01-22 | US5243316A | 1993-09-07 | Hiroshi Sakakima; Mitsuo Satomi; Toshio Takada; Teruya Shinjo |
There is provided a magnetoresistance effect element which is a multilayer structure body wherein a first magnetic film layer made of Ni-rich Ni-Co-Fe having a thickness of 10 to 100 .ANG. and a second magnetic film layer made of Co-rich Co-Ni-Fe having a thickness of 10 to 100 .ANG., which are different from each other in coercive force, are integrally laminated with a non-magnetic metal film layer having a thickness of 10 to 100 .ANG. interposed therebetween. The non-magnetic metal film layer is of a metal, for example, Cu, Ag, Au, Pt, Ru or Re. (Ni.sub.A Co.sub.1-A).sub.B Fe.sub.1-B, Ni.sub.A Fe.sub.1-A or Ni.sub.A Co.sub.1-A is used as a material of the first magnetic film, and (Co.sub.C Ni.sub.1-C).sub.D Fe.sub.1-D is used as a material of the second magnetic film. | ||||||
113 | Flux spreading thin film magnetic devices | US360421 | 1989-06-02 | US5085935A | 1992-02-04 | Michael L. Mallary |
One aspect of the invention is a method of flux conduction comprising providing a structure with anisotropy not purely in the transverse in-plane direction such that flux spreading into the transverse in-plane direction can occur by rotation. Apparatus includes a thin film magnetic recording device having at least one pole with two magnetic layers and capable of conducting signal flux, a first of the magnetic layers having domains oriented in a first direction, a second of said magnetic layers having domains oriented in a second distinct direction, the layers coupled to each other such that signal flux can flow therebetween. Method of making and various embodiments disclosed. | ||||||
114 | Magnetic nitride film | US445105 | 1989-12-07 | US5049209A | 1991-09-17 | Hiroshi Sakakima; Koichi Osano; Yuji Omata; Mitsuo Satomi; Koichi Kugimiya |
The disclosed magnetic nitride T-M-N film (T is at least one metal selected from the group consisting of Fe, Co, Ni and Mn; M is at least one metal selected from the group consisting of Nb, Zr, Ti, Ta, Hf, Cr, W and Mo; N is nitrogen (N)) has excellent wear resistance and high electric resistivity, and the compositionally modulated nitride film shows a soft magnetic property, as well as thermal stability of the properties. | ||||||
115 | Method of manufacturing crystalline thin-film of rare-earth compounds | US497894 | 1990-03-22 | US5041200A | 1991-08-20 | Hiromitsu Ishii; Tsuneharu Takeda; Kyuya Baba; Ikuhiro Yamaguchi |
Gd and Bi are used as sputter sources and are simultaneously sputtered, or sputtered alternately, each time in an amount for forming a layer having a thickness of 10 atoms or less, thereby forming a thin film on a substrate, in which Gd and Bi are mixed at a ratio of 4:3. The thin film is heat-treated to form a crystalline thin film having a phase represented by Gd.sub.4 Bi.sub.3. | ||||||
116 | Magneto-optical recording medium | US748580 | 1985-06-25 | US4701881A | 1987-10-20 | Fujio Tanaka; Nobutake Imamura |
A magneto-optical recording medium is disclosed in which a magnetic thin film recording layer is formed by a magnetic material having a Curie temperature or magnetic compensation temperature as low as 50.degree. to 250.degree. C. and a coercive force as large as 1 KOe or more and having an easy axis of magnetization perpendicularly to the film surface. A substantially transparent magnetic material film layer of ferrite, garnet or the like is disposed adjacent the recording film layer, large in the Faraday rotation angle and having an easy axis of magnetization perpendicularly to the film surface. A transparent substrate is disposed on the side of incidence of light. The substantially transparent magnetic material layer of the ferrite, garnet or the like may increase the magneto-optical rotation angle in the magnetic thin film recording layer, or may increase the magneto-optical rotation angle by the Faraday effect. The thickness of the substantially transparent magnetic material layer is selected in such a region where the figure of merit .sqroot.R.multidot..theta..sub.k expressed by its reflectivity R and the magneto-optical rotation angle .theta..sub.k is maximum. | ||||||
117 | Multi-layered ferromagnetic film and method of manufacturing the same | US918333 | 1986-10-14 | US4698273A | 1987-10-06 | Matahiro Komuro; Yuzo Kozono; Takeshi Yasuda; Shinji Narishige; Masanobu Hanazono; Tetsuro Kuroda |
The film is composed of an alternate lamination of unit iron layers and unit layers of ferromagnetic iron compound such as Fe.sub.3 Al, Fe.sub.3 Si, Fe.sub.3 Ge and Fe.sub.3 Ga. The thickness of the both unit layers is less than 70 .ANG.. The film has a high saturation magnetization more than 230 emu/g and a high thermal stability so that the film is particularly applicable to a magnetic head core. | ||||||
118 | Flexible magnetic recording medium comprising an underlying film having reduced in-plane magnetic anisotropy under a surface film having perpendicular magnetic anisotropy | US710923 | 1985-03-12 | US4657819A | 1987-04-14 | Hidefumi Funaki |
In a flexible magnetic recording medium comprising first and second films (11) and (12) successively formed on a substrate (10), the first film comprises an alloy of nickel and iron together with a magnetization adjusting component. An amount of the magnetization adjusting component is adjusted so that the first film has saturation magnetization less than or equal to 500 e.m.u./cc. The magnetization adjusting component may be either molybdenum or a combination of molybdenum and copper. The magnetization adjusting component may be between 12 and 50% by weight in the first film. Alternatively, the magnetization adjusting component may be titanium or silicon. The alloy may be Permalloy. The substrate may be a polyester film. | ||||||
119 | Intermediary layers for epitaxial hexagonal ferrite films | US720202 | 1985-04-04 | US4624901A | 1986-11-25 | Howard L. Glass |
A single crystal film of a hexagonal ferrite is deposited on a nonmagnetic, single crystal substrate with a film of a second ferrite material interposed between the substrate and the hexagonal ferrite film. In a preferred embodiment, the substrate is of nonmagnetic spinel and the second ferrite material is a spinel ferrite. | ||||||
120 | Magnetic films having a predetermined coercivity | US3700500D | 1967-12-04 | US3700500A | 1972-10-24 | RODBELL DONALD STANLEY; LOMMEL JAMES M |
D R A W I N G
MAGNETIC FILMS HAVING A PREDETERMINED COERCIVITY ARE FORMED BY DISPOSING A VACUUM DEPOSITED, POLYCRYSTALLINE THIN MAGNETIC FILM OF IRON, COBALT OR NICKEL IN AN OXYGEN BEARING ATMOSPHERE AND SUBSEQUENTLY ANNEALING THE MAGNETIC FILM AT A TEMPERATURE BETWEEN 50*C. AND 600*C. FOR A SUFFICIENT PERIOD, E.G. BETWEEN 10 TO 300 MINUTES, TO INCREASE THE COERCIVITY OF THE MAGNETIC FILM TO A DESIRED VALUE WITHIN A FIXED RANGE. IN A SPECIFIC INSTANCE, A MONOTONIC INCREASE FROM 38.4 OERSTEDS TO 530 OERSTEDS WAS OBSERVED IN THE COERCIVE FORCE OF 300 A. THICK IRON FILM UPON A GLASS SUBSTRATE WHEN ANNEALED FOR 130 MINUTES AT A PRESSURE OF 5X10**-5 TORR. ANNEALING OF THE MAGNETIC FILMS GENERALLY WAS FOUND TO PRODUCE ONLY A FRACTIONAL DECREASE IN THE MAGNETIZATION OF THE FILMS. |