JPH08106664A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPH08106664A
JPH08106664A JP6242841A JP24284194A JPH08106664A JP H08106664 A JPH08106664 A JP H08106664A JP 6242841 A JP6242841 A JP 6242841A JP 24284194 A JP24284194 A JP 24284194A JP H08106664 A JPH08106664 A JP H08106664A
Authority
JP
Japan
Prior art keywords
magnetic
thin film
core
magnetic core
head
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP6242841A
Other languages
Japanese (ja)
Inventor
Koji Fusayasu
浩嗣 房安
Hiroto Inoue
裕人 井ノ上
Tatsuhiko Inagaki
辰彦 稲垣
Hiroshi Takaso
洋 高祖
Makoto Kuwamoto
誠 桑本
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP6242841A priority Critical patent/JPH08106664A/en
Publication of JPH08106664A publication Critical patent/JPH08106664A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10532Heads
    • G11B11/10541Heads for reproducing
    • G11B11/10543Heads for reproducing using optical beam of radiation
    • G11B11/10547Heads for reproducing using optical beam of radiation interacting with the magnetisation of an intermediate transfer element, e.g. magnetic film, included in the head

Abstract

(57)【要約】 【目的】 光学的に磁気情報を再生する磁気ヘッドに関
するもので、磁気光学材料よりなる磁性薄膜に磁束を集
中させることにより、磁性薄膜表面の磁化の回転角度が
大きくなり高出力の再生信号が得られ、高密度記録にお
ける再生感度を格段に向上できる磁気ヘッドを提供す
る。 【構成】 磁気記録媒体6の面側に磁気ギャップ5を有
し、磁気ギャップ5を介して第1の磁気コア1と第2の
磁気コア2が対面しており、第1の磁気コア1と前記第
2の磁気コア2とを連結する磁気光学材料からなる磁性
薄膜3とによって閉磁路12が形成されている磁気ヘッ
ドであって、磁性薄膜3に沿って磁束集中部材としての
導電性部材4が配設されている。
(57) [Abstract] [Purpose] A magnetic head that optically reproduces magnetic information. By concentrating a magnetic flux on a magnetic thin film made of a magneto-optical material, the rotation angle of magnetization on the surface of the magnetic thin film increases and (EN) A magnetic head capable of obtaining an output reproduction signal and significantly improving reproduction sensitivity in high density recording. A magnetic gap 5 is provided on the surface side of a magnetic recording medium 6, and a first magnetic core 1 and a second magnetic core 2 face each other with the magnetic gap 5 in between. A magnetic head in which a closed magnetic path 12 is formed by a magnetic thin film 3 made of a magneto-optical material that connects the second magnetic core 2 and a conductive member 4 as a magnetic flux concentrating member along the magnetic thin film 3. Is provided.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、磁気記録媒体に磁気記
録された情報を光学的に再生する磁気ヘッドに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic head for optically reproducing information magnetically recorded on a magnetic recording medium.

【0002】[0002]

【従来の技術】近年、情報通信・映像音響の各分野で、
高密度(小型・大容量)な情報記録再生装置が盛んに開
発されている。
2. Description of the Related Art Recently, in the fields of information communication and audiovisual,
High-density (small size / large capacity) information recording / reproducing devices are being actively developed.

【0003】その中でも磁気記録の進歩はめざましく、
高記録密度化、小型化、転送速度の高速化が進み、記録
密度は10年で約10倍の向上が図られている。
Among them, the progress of magnetic recording is remarkable,
The recording density has been increased, the size has been reduced, and the transfer speed has been increased, and the recording density has been improved about 10 times in 10 years.

【0004】現在、磁気ディスク装置に広く応用されて
いる長手磁化方式の高密度記録において、最短のビット
間隔を短くし、線記録密度を向上させるためには、記録
レベルをできるだけ低くして、媒体の表面層だけを浅く
磁化するか、媒体の磁性層厚を最短のビット間隔の2分
の1(4分の1波長)以下に薄くして、できるだけ高密
度まで円弧状磁化モードを保つことが必要である。
In the high density recording of the longitudinal magnetization system which is currently widely applied to magnetic disk devices, in order to shorten the shortest bit interval and improve the linear recording density, the recording level should be as low as possible. It is possible to keep the arc-shaped magnetization mode as high as possible by either shallowly magnetizing only the surface layer or thinning the magnetic layer thickness of the medium to less than half (1/4 wavelength) of the shortest bit interval. is necessary.

【0005】また、トラックピッチを小さくし、トラッ
ク記録密度を向上させるためには、ヘッドを任意のトラ
ックへ高速高精度に位置決めすることと、ビット長に合
わせて、1ビット記録面積が小さくなることから、ヘッ
ドが、媒体からの周波数の高い小さな磁界を高感度に検
出することが必要である。
In order to reduce the track pitch and improve the track recording density, the head is positioned on an arbitrary track at high speed and with high precision, and the 1-bit recording area is reduced according to the bit length. Therefore, it is necessary for the head to detect a small high-frequency magnetic field from the medium with high sensitivity.

【0006】すなわち、長手磁化方式による磁気記録の
高密度記録再生の課題としては、 再生ヘッドの高感度化 記録再生ヘッド位置決めの高速高精度化 磁気記録媒体の高保持力化と記録ヘッドの高出力化 が挙げられる。
That is, as the problems of high density recording / reproducing of magnetic recording by the longitudinal magnetization method, high sensitivity of the reproducing head, high speed and high accuracy of positioning of the recording / reproducing head, high coercive force of the magnetic recording medium and high output of the recording head. There is a change.

【0007】しかし、媒体の高保持力化は記録ヘッドの
書き込み能力で制限されるだけでなく、読み出し時の諸
損失のため高密度ほど再生電圧は急激に減衰し、実用で
きる記録密度は理論値に比べかなり下回っているのが現
状である。
However, the increase in the holding power of the medium is not only limited by the writing ability of the recording head, but also the reproduction voltage is rapidly attenuated as the density is increased due to various losses during reading, and the practical recording density is the theoretical value. The current situation is much lower than

【0008】すなわち、磁気記録の高密度化には記録ヘ
ッドの書き込み能力を向上させるとともに、再生ヘッド
の再生感度を向上させることが必須である。
That is, in order to increase the density of magnetic recording, it is essential to improve the writing ability of the recording head and the reproduction sensitivity of the reproducing head.

【0009】そこで、長手磁化(面内磁化)方式の磁化
信号再生方法として、強磁性体薄膜に媒体磁化信号を転
写し、その強磁性体薄膜の磁気光学効果を応用した方式
が提案されている(例えば、特公昭56−33781号
公報、特開昭61−214258号公報、特公平3−5
5894号公報)。
Therefore, as a longitudinal magnetization (in-plane magnetization) method of reproducing a magnetization signal, a method has been proposed in which a medium magnetization signal is transferred to a ferromagnetic thin film and the magneto-optical effect of the ferromagnetic thin film is applied. (For example, JP-B-56-33781, JP-A-61-214258, and JP-B-3-5.
5894).

【0010】以下、図面を参照しながら、従来の磁気ヘ
ッドの一例について説明する。
An example of a conventional magnetic head will be described below with reference to the drawings.

【0011】図5は従来の磁気ヘッドの原理を示す断面
図である。図5において、1は第1の磁気コア、2は第
2の磁気コア、5は磁気ギャップ(通常はガラスからな
る)、6は磁気記録媒体、16は磁気光学材料からなる
磁性体である。第1の磁気コア1と第2の磁気コア2は
磁気ギャップ5を介して対面しており、磁気記録媒体6
に記録された情報信号記録による磁化13から発生した
磁束は第1の磁気コア1、第2の磁気コア2および磁気
光学材料からなる磁性体16によって閉磁路12を形成
している。
FIG. 5 is a sectional view showing the principle of a conventional magnetic head. In FIG. 5, 1 is a first magnetic core, 2 is a second magnetic core, 5 is a magnetic gap (usually made of glass), 6 is a magnetic recording medium, and 16 is a magnetic body made of a magneto-optical material. The first magnetic core 1 and the second magnetic core 2 face each other via the magnetic gap 5, and the magnetic recording medium 6
The magnetic flux generated from the magnetization 13 due to the information signal recording recorded in (1) forms the closed magnetic path 12 by the first magnetic core 1, the second magnetic core 2 and the magnetic body 16 made of a magneto-optical material.

【0012】以上のように構成された磁気ヘッドについ
て、以下、図5を用いてその動作を説明する。
The operation of the magnetic head having the above structure will be described below with reference to FIG.

【0013】磁気記録媒体6の情報信号記録による磁化
13の大きさと方向とによって、磁気ヘッド中に設けら
れた磁気光学材料からなる磁性体16の磁化が変化し、
その磁性体16に偏向された光を入射すると、磁化の大
きさと方向とによって偏光面が回転し、光検出器によっ
てその反射光の偏光角を電気信号として検出する。
Depending on the magnitude and direction of the magnetization 13 due to the information signal recording of the magnetic recording medium 6, the magnetization of the magnetic body 16 made of a magneto-optical material provided in the magnetic head changes.
When the polarized light is incident on the magnetic body 16, the plane of polarization is rotated depending on the magnitude and direction of the magnetization, and the photodetector detects the polarization angle of the reflected light as an electric signal.

【0014】[0014]

【発明が解決しようとする課題】しかしながら、上述の
ような構成では、高密度記録された媒体を再生しようと
する場合、再生信号が低下するという問題を有してい
た。すなわち、1ビット記録面積が小さくなり、磁気記
録媒体6の情報信号記録による磁化13の大きさは小さ
くなる。また、磁気ヘッド中に設けられた磁気光学材料
からなる磁性体16のため磁気ヘッドの磁気抵抗は大き
くなり、磁気コアの漏れ磁束が増大し磁気光学材料から
なる磁性体16での有効磁束は低下する。その結果、磁
性体16での磁化の大きさと方向との変化量が小さくな
り出力が低下する。さらに、磁気ヘッドの磁気抵抗を低
減させるために磁気光学材料からなる磁性体16の厚み
を厚くすると、その磁性体の磁束密度が低下し磁化の大
きさと方向との変化量が小さくなり出力が低下するとい
う問題を有していた。
However, the above-mentioned structure has a problem that the reproduction signal is lowered when reproducing a medium recorded at high density. That is, the 1-bit recording area becomes small, and the size of the magnetization 13 due to the information signal recording on the magnetic recording medium 6 becomes small. Further, since the magnetic body 16 made of the magneto-optical material provided in the magnetic head increases the magnetic resistance of the magnetic head, the leakage magnetic flux of the magnetic core increases, and the effective magnetic flux in the magnetic body 16 made of the magneto-optical material decreases. To do. As a result, the amount of change in the magnitude and direction of the magnetization in the magnetic body 16 is reduced, and the output is reduced. Further, if the thickness of the magnetic body 16 made of a magneto-optical material is increased in order to reduce the magnetic resistance of the magnetic head, the magnetic flux density of the magnetic body is reduced and the amount of change in the magnitude and direction of the magnetization is reduced, so that the output is reduced. Had the problem of doing.

【0015】本発明は、上記したような事情に鑑み、従
来の方式に比べ高密度記録における再生感度を格段に向
上できる磁気ヘッドを提供することを目的とする。
In view of the above circumstances, it is an object of the present invention to provide a magnetic head capable of remarkably improving the reproducing sensitivity in high density recording as compared with the conventional method.

【0016】[0016]

【課題を解決するための手段】本発明に係る第1の磁気
ヘッドは、磁気記録媒体面側に磁気ギャップを有し、前
記磁気ギャップを介して第1の磁気コアと第2の磁気コ
アが対面しており、前記第1の磁気コアと前記第2の磁
気コアとこれら両磁気コアを連結する磁気光学材料から
なる磁性薄膜とによって閉磁路が形成されている磁気ヘ
ッドであって、前記磁性薄膜に沿って磁束集中部材が配
設されていることを特徴とするものである。
A first magnetic head according to the present invention has a magnetic gap on the surface side of a magnetic recording medium, and the first magnetic core and the second magnetic core are connected via the magnetic gap. A magnetic head that faces each other and has a closed magnetic path formed by the first magnetic core, the second magnetic core, and a magnetic thin film made of a magneto-optical material that connects both magnetic cores. The magnetic flux concentrating member is arranged along the thin film.

【0017】また、本発明に係る第2の磁気ヘッドは、
磁気記録媒体面側に磁気ギャップを有し、前記磁気ギャ
ップを介して第1の磁気コアと第2の磁気コアが対面し
ており、前記第1の磁気コアと前記第2の磁気コアとこ
れら両磁気コアを連結する磁気光学材料からなる磁性薄
膜とによって閉磁路が形成されている磁気ヘッドであっ
て、前記第1の磁気コアの前記第2の磁気コアに対面す
る面、あるいは前記第2の磁気コアの前記第1の磁気コ
アに対面する面の少なくとも一方に磁気遮蔽部材が配設
されていることを特徴とするものである。
The second magnetic head according to the present invention is
A magnetic gap is provided on the surface side of the magnetic recording medium, and the first magnetic core and the second magnetic core face each other through the magnetic gap, and the first magnetic core and the second magnetic core A magnetic head in which a closed magnetic path is formed by a magnetic thin film made of a magneto-optical material that connects both magnetic cores, wherein the surface of the first magnetic core faces the second magnetic core, or the second magnetic core. The magnetic shielding member is disposed on at least one of the surfaces of the magnetic core facing the first magnetic core.

【0018】[0018]

【作用】本発明に係る第1の磁気ヘッドにおいては、磁
性薄膜に沿った磁束集中部材の存在により磁気光学材料
からなる磁性薄膜に磁束が集中し、磁性薄膜表面の磁化
の回転角度が大きくなり高出力の再生信号が得られ、高
密度記録における再生感度が向上する。
In the first magnetic head according to the present invention, the presence of the magnetic flux concentrating member along the magnetic thin film concentrates the magnetic flux on the magnetic thin film made of the magneto-optical material, thereby increasing the rotation angle of the magnetization on the surface of the magnetic thin film. A reproduction signal of high output is obtained, and reproduction sensitivity in high density recording is improved.

【0019】また、本発明に係る第2の磁気ヘッドにお
いては、磁気コアどうしの対面する面に配設した磁気遮
蔽部材の存在により磁気ギャップ近傍の漏れ磁束が低減
し、磁性薄膜での磁化の回転角度が大きくなり、再生出
力が大きくなる。
Further, in the second magnetic head according to the present invention, the presence of the magnetic shielding member arranged on the surfaces of the magnetic cores facing each other reduces the leakage magnetic flux in the vicinity of the magnetic gap and reduces the magnetization of the magnetic thin film. The rotation angle becomes large and the reproduction output becomes large.

【0020】[0020]

【実施例】本発明の磁気ヘッドの実施例について、図面
を参照しながら説明する。
Embodiments of the magnetic head of the present invention will be described with reference to the drawings.

【0021】(第1の実施例)以下、本発明における第
1の実施例の磁気ヘッドについて図面を参照しながら説
明する。
(First Embodiment) A magnetic head according to the first embodiment of the present invention will be described below with reference to the drawings.

【0022】図1は、第1の実施例の磁気ヘッドを示す
斜視図である。図2は図1の分断線C−Dに沿った断面
図である。図1、図2において、1は第1の磁気コア、
2は第2の磁気コア、3は磁気光学材料からなる磁性薄
膜(例えば厚さ20nmの電子ビーム蒸着したパーマロ
イ膜)、4は磁束集中部材としての渦電流の生じる導電
性部材(例えば銅)、5は通常はガラスからなる磁気ギ
ャップ、6は磁気記録媒体、7は光源、8は入射光、9
はハーフミラー、10は反射光、11は受光素子であ
る。第1の磁気コア1と第2の磁気コア2は磁気記録媒
体6側に配設された磁気ギャップ5を介して対面してお
り、磁気記録媒体6に記録された情報信号記録による磁
化13から発生した磁束は第1の磁気コア1、第2の磁
気コア2および磁気光学材料からなる磁性薄膜3によっ
て閉磁路12を形成しており、その磁性薄膜3の下面に
沿って磁束集中部材としての導電性部材4が配設されて
いる。
FIG. 1 is a perspective view showing the magnetic head of the first embodiment. FIG. 2 is a sectional view taken along the section line CD of FIG. 1 and 2, 1 is the first magnetic core,
Reference numeral 2 is a second magnetic core, 3 is a magnetic thin film made of a magneto-optical material (for example, a permalloy film vapor-deposited with an electron beam having a thickness of 20 nm), 4 is a conductive member (for example, copper) that generates an eddy current as a magnetic flux concentration member, 5 is a magnetic gap usually made of glass; 6 is a magnetic recording medium; 7 is a light source; 8 is incident light;
Is a half mirror, 10 is reflected light, and 11 is a light receiving element. The first magnetic core 1 and the second magnetic core 2 face each other via a magnetic gap 5 arranged on the magnetic recording medium 6 side, and from the magnetization 13 recorded on the magnetic recording medium 6 by the information signal recording. The generated magnetic flux forms a closed magnetic circuit 12 by the first magnetic core 1, the second magnetic core 2 and the magnetic thin film 3 made of a magneto-optical material, and along the lower surface of the magnetic thin film 3 serves as a magnetic flux concentrating member. A conductive member 4 is provided.

【0023】以上のように構成された磁気ヘッドについ
て、以下、図1および図2を用いてその動作を説明す
る。
The operation of the magnetic head configured as described above will be described below with reference to FIGS. 1 and 2.

【0024】磁気ヘッド内部の閉磁路12の方向は、磁
気記録媒体6の高速移動に伴い高速に反転を繰り返すた
め、磁束集中部材としての導電性部材4の内部には渦電
流が発生し、反作用磁界が生じる。その結果、磁性薄膜
3では漏れ磁束が減少するとともに、その内部の磁束は
上部(光が入射する側)に集中し、その磁界の強さは大
きくなり、磁性薄膜3の表面の磁化の回転角度は大きく
なる。
Since the direction of the closed magnetic path 12 inside the magnetic head is repeatedly reversed at high speed as the magnetic recording medium 6 moves at high speed, an eddy current is generated inside the conductive member 4 as a magnetic flux concentrating member, which causes a reaction. A magnetic field is generated. As a result, the magnetic flux in the magnetic thin film 3 is reduced, and the magnetic flux inside the magnetic thin film 3 is concentrated on the upper side (the side on which light is incident), the magnetic field strength is increased, and the rotation angle of the magnetization of the surface of the magnetic thin film 3 is increased. Grows.

【0025】磁性薄膜3における閉磁路12と磁化14
の関係を、図2のE方向矢視図である図3を用いて説明
する。図3に示すように磁性薄膜3での磁路12の方向
により、その磁化14は回転する。磁路が12Fの方向
のとき磁化は14Fのように回転し、磁路が12Gの方
向のとき磁化は14Gのように回転し、磁性薄膜3の磁
界の強さが大きいほどその回転の角度は大きくなり、再
生出力は大きくなる。
Closed magnetic path 12 and magnetization 14 in the magnetic thin film 3.
2 will be described with reference to FIG. 3, which is a view taken in the direction of arrow E in FIG. As shown in FIG. 3, the magnetization 14 rotates depending on the direction of the magnetic path 12 in the magnetic thin film 3. When the magnetic path is in the direction of 12F, the magnetization rotates like 14F, and when the magnetic path is in the direction of 12G, the magnetization rotates like 14G. As the magnetic field strength of the magnetic thin film 3 increases, the angle of rotation increases. The playback output is increased.

【0026】また、磁性薄膜3の厚さが厚くなっても、
磁束集中部材としての導電性部材4に発生する反作用磁
界のために、磁性薄膜3の上部(光が入射する側)の磁
束密度は低下せず、磁化の回転角度は小さくならず出力
も低下しない。このように磁気ヘッド内部の磁路12の
大きさと方向との変化によって磁性薄膜3の磁化14は
回転する。光源7より発生する偏向された入射光8は、
磁性薄膜3で磁気光学効果によって偏光の向きが回転す
る。その反射光10はハーフミラー9で反射し、受光素
子11で電気信号に変換され、再生出力が得られる。
Even if the magnetic thin film 3 becomes thick,
Due to the reaction magnetic field generated in the conductive member 4 as the magnetic flux concentrating member, the magnetic flux density in the upper part (on the side where light is incident) of the magnetic thin film 3 does not decrease, the rotation angle of magnetization does not decrease, and the output does not decrease. . In this way, the magnetization 14 of the magnetic thin film 3 is rotated by the change in the size and direction of the magnetic path 12 inside the magnetic head. The deflected incident light 8 generated from the light source 7 is
The direction of polarized light is rotated by the magnetic thin film 3 by the magneto-optical effect. The reflected light 10 is reflected by the half mirror 9, converted into an electric signal by the light receiving element 11, and a reproduction output is obtained.

【0027】なお、本実施例では、磁性薄膜を20nm
のパーマロイ膜としたが、磁気光学効果を有する他の磁
性薄膜でも、また他の膜厚でも同様の効果を有する。
In this embodiment, the magnetic thin film has a thickness of 20 nm.
However, other magnetic thin films having a magneto-optical effect and other film thicknesses have the same effect.

【0028】また、本実施例では、磁気光学材料からな
る磁性薄膜内に磁束を集中させるための磁束集中部材と
しての導電性部材として銅を配置したが、高導電率を有
する他の導電性部材でも、マイスナー効果を有する超電
導部材でも同様の効果を有する。
Further, in the present embodiment, copper is arranged as the conductive member as the magnetic flux concentrating member for concentrating the magnetic flux in the magnetic thin film made of the magneto-optical material, but another conductive member having high conductivity is used. However, a superconducting member having a Meissner effect also has the same effect.

【0029】(第2の実施例)以下、本発明における第
2の実施例の磁気ヘッドについて図面を参照しながら説
明する。
(Second Embodiment) A magnetic head according to a second embodiment of the present invention will be described below with reference to the drawings.

【0030】図4は、第2の実施例の磁気ヘッドを示す
断面図である。図4において、15は磁気遮蔽部材とし
ての例えば銅のような渦電流の生じる導電性部材であ
り、第1の磁気コア1の第2の磁気コア2に対面する面
と第2の磁気コア2の第1の磁気コア1に対面する面に
渦電流の生じる導電性部材15が配設されている点が第
1の実施例とは異なり、それ以外は前述した第1の実施
例と同じであるので同一の符号を付し、説明は割愛す
る。
FIG. 4 is a sectional view showing the magnetic head of the second embodiment. In FIG. 4, reference numeral 15 denotes a conductive member, such as copper, that generates an eddy current as a magnetic shield member. The conductive member 15 faces the second magnetic core 2 of the first magnetic core 1 and the second magnetic core 2. Is different from the first embodiment in that a conductive member 15 for generating an eddy current is arranged on the surface facing the first magnetic core 1, and other points are the same as the above-described first embodiment. Therefore, the same reference numerals are given and the description will be omitted.

【0031】以上のように構成された磁気ヘッドについ
て、以下、図4を用いてその動作を説明する。
The operation of the magnetic head having the above structure will be described below with reference to FIG.

【0032】第1の実施例では、磁気光学材料からなる
磁性薄膜3の厚さが20nmと極端に薄いために磁気抵
抗が大きくなり、磁気ギャップ5の近傍で漏れ磁束が大
きくなり、磁性薄膜3の有効磁束が減少し磁化の回転角
度が小さくなるという傾向を内包している。
In the first embodiment, the magnetic thin film 3 made of a magneto-optical material has an extremely thin thickness of 20 nm, so that the magnetic resistance becomes large, the leakage magnetic flux becomes large in the vicinity of the magnetic gap 5, and the magnetic thin film 3 is formed. It has a tendency that the effective magnetic flux of is decreased and the rotation angle of the magnetization is decreased.

【0033】これに対して、本実施例では、第1の磁気
コア1の第2の磁気コア2に対面する面と第2の磁気コ
ア2の第1の磁気コア1に対面する面に磁気遮蔽部材と
しての導電性部材15を設けることで、渦電流による反
作用磁界で磁気ギャップ5の近傍の漏れ磁束を低減させ
るため、磁性薄膜3での磁化の回転角度は大きくなり、
再生出力は大きくなる。
On the other hand, in this embodiment, the surface of the first magnetic core 1 facing the second magnetic core 2 and the surface of the second magnetic core 2 facing the first magnetic core 1 are magnetized. By providing the conductive member 15 as the shield member, the leakage magnetic flux in the vicinity of the magnetic gap 5 is reduced by the reaction magnetic field due to the eddy current, so that the rotation angle of the magnetization in the magnetic thin film 3 increases.
The reproduction output becomes large.

【0034】なお、本実施例では、磁性薄膜を20nm
のパーマロイ膜としたが、磁気光学効果を有する他の磁
性薄膜でも、また他の膜厚でも同様の効果を有する。
In this embodiment, the magnetic thin film is 20 nm thick.
However, other magnetic thin films having a magneto-optical effect and other film thicknesses have the same effect.

【0035】また、本実施例では第1の磁気コアの第2
の磁気コアに対面する面と第2の磁気コアの第1の磁気
コアに対面する面に漏れ磁束を防ぐために磁気遮蔽部材
としての導電性部材として銅を配置したが、高導電率を
有する他の導電性部材でも、マイスナー効果を有する超
電導部材でも同様の効果を有する。
In this embodiment, the second magnetic core of the first magnetic core is used.
Copper is arranged as a conductive member as a magnetic shielding member on the surface of the second magnetic core facing the first magnetic core and the surface of the second magnetic core facing the first magnetic core. The same effect can be obtained by either the conductive member or the superconducting member having the Meissner effect.

【0036】また、本実施例では第1の磁気コアの第2
の磁気コアに対面する面と第2の磁気コアの第1の磁気
コアに対面する面の両方に漏れ磁束を防ぐために渦電流
の生じる導電性部材を配置したが、一方の面のみに導電
性部材を配置しても同様の効果を有する。
In this embodiment, the second magnetic core of the first magnetic core is also used.
Of the second magnetic core and the surface of the second magnetic core facing the first magnetic core are each provided with a conductive member in which an eddy current is generated in order to prevent a leakage magnetic flux, but only one surface is made conductive. Even if the members are arranged, the same effect can be obtained.

【0037】また、本実施例では磁気光学材料からなる
磁性薄膜内に磁束を集中させるための磁束集中部材を伴
った磁気ヘッドに、第1の磁気コアの第2の磁気コアに
対面する面と第2の磁気コアの第1の磁気コアに対面す
る面に漏れ磁束を防ぐために磁気遮蔽部材を配置した
が、磁束集中部材を伴わない磁気ヘッドでも同様の効果
を有する。
Further, in this embodiment, the magnetic head having a magnetic flux concentrating member for concentrating the magnetic flux in the magnetic thin film made of the magneto-optical material is provided with a surface facing the second magnetic core of the first magnetic core. Although the magnetic shield member is arranged on the surface of the second magnetic core facing the first magnetic core in order to prevent the leakage magnetic flux, a magnetic head having no magnetic flux concentrating member has the same effect.

【0038】[0038]

【発明の効果】本発明に係る第1の磁気ヘッドによれ
ば、磁性薄膜に沿った磁束集中部材の存在により磁気光
学材料からなる磁性薄膜に磁束を集中させるため、磁性
薄膜表面の磁化の回転角度が大きくなって高出力の再生
信号が得られ、高密度記録における再生感度を格段に向
上することができる。
According to the first magnetic head of the present invention, since the magnetic flux is concentrated on the magnetic thin film made of the magneto-optical material due to the presence of the magnetic flux concentration member along the magnetic thin film, the rotation of the magnetization of the surface of the magnetic thin film is rotated. As the angle becomes larger, a high output reproduction signal can be obtained, and the reproduction sensitivity in high density recording can be remarkably improved.

【0039】また、本発明に係る第2の磁気ヘッドによ
れば、磁気コアどうしの対面する面に配設した磁気遮蔽
部材の存在により磁気ギャップ近傍の漏れ磁束を低減す
るので、磁性薄膜での磁化の回転角度が大きくなって高
出力の再生信号が得られ、高密度記録における再生感度
を格段に向上することができる。
Further, according to the second magnetic head of the present invention, since the magnetic flux leakage near the magnetic gap is reduced by the presence of the magnetic shielding member arranged on the surfaces of the magnetic cores facing each other, the magnetic thin film The rotation angle of the magnetization is increased to obtain a high output reproduction signal, and the reproduction sensitivity in high density recording can be significantly improved.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の第1の実施例における磁気ヘッドを説
明する斜視図である。
FIG. 1 is a perspective view illustrating a magnetic head according to a first embodiment of the invention.

【図2】本発明の第1の実施例における磁気ヘッドを説
明する断面図である。
FIG. 2 is a sectional view illustrating a magnetic head according to the first embodiment of the invention.

【図3】本発明の磁気光学効果を有する磁性薄膜表面に
おける磁化の方向を説明する矢視図である。
FIG. 3 is a view for explaining the direction of magnetization on the surface of the magnetic thin film having the magneto-optical effect of the present invention.

【図4】本発明の第2の実施例における磁気ヘッドを説
明する断面図である。
FIG. 4 is a sectional view illustrating a magnetic head according to a second embodiment of the present invention.

【図5】従来の磁気ヘッドを説明する断面図である。FIG. 5 is a sectional view illustrating a conventional magnetic head.

【符号の説明】[Explanation of symbols]

1……第1の磁気コア 2……第2の磁気コア 3……磁気光学材料からなる磁性薄膜 4……導電性部材(磁束集中部材) 5……磁気ギャップ 6……磁気記録媒体 7……光源 8……入射光 9……ハーフミラー 10……反射光 11……受光素子 12……閉磁路 13……磁化 14……磁化 15……導電性部材(磁気遮蔽部材) 16……磁気光学材料からなる磁性体 1 ... First magnetic core 2 ... Second magnetic core 3 ... Magnetic thin film made of magneto-optical material 4 ... Conductive member (magnetic flux concentrating member) 5 ... Magnetic gap 6 ... Magnetic recording medium 7 ... ... Light source 8 ... Incident light 9 ... Half mirror 10 ... Reflected light 11 ... Light receiving element 12 ... Closed magnetic path 13 ... Magnetization 14 ... Magnetization 15 ... Conductive member (magnetic shielding member) 16 ... Magnetic Magnetic material made of optical material

───────────────────────────────────────────────────── フロントページの続き (72)発明者 高祖 洋 大阪府門真市大字門真1006番地 松下電器 産業株式会社内 (72)発明者 桑本 誠 大阪府門真市大字門真1006番地 松下電器 産業株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Hiroshi Sozo 1006 Kadoma, Kadoma City, Osaka Prefecture Matsushita Electric Industrial Co., Ltd. (72) Makoto Kuwamoto 1006 Kadoma, Kadoma City, Osaka Matsushita Electric Industrial Co., Ltd.

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】 磁気記録媒体面側に磁気ギャップを有
し、前記磁気ギャップを介して第1の磁気コアと第2の
磁気コアが対面しており、前記第1の磁気コアと前記第
2の磁気コアとこれら両磁気コアを連結する磁気光学材
料からなる磁性薄膜とによって閉磁路が形成されている
磁気ヘッドであって、前記磁性薄膜に沿って磁束集中部
材が配設されていることを特徴とする磁気ヘッド。
1. A magnetic recording medium has a magnetic gap on the surface side, and a first magnetic core and a second magnetic core face each other via the magnetic gap, and the first magnetic core and the second magnetic core face each other. A magnetic head in which a closed magnetic path is formed by a magnetic core and a magnetic thin film made of a magneto-optical material connecting both magnetic cores, wherein a magnetic flux concentrating member is arranged along the magnetic thin film. Characteristic magnetic head.
【請求項2】 磁束集中部材は、導電性材料からなるこ
とを特徴とする請求項1に記載の磁気ヘッド。
2. The magnetic head according to claim 1, wherein the magnetic flux concentration member is made of a conductive material.
【請求項3】 磁束集中部材は、超電導材料からなるこ
とを特徴とする請求項1に記載の磁気ヘッド。
3. The magnetic head according to claim 1, wherein the magnetic flux concentrating member is made of a superconducting material.
【請求項4】 磁気記録媒体面側に磁気ギャップを有
し、前記磁気ギャップを介して第1の磁気コアと第2の
磁気コアが対面しており、前記第1の磁気コアと前記第
2の磁気コアとこれら両磁気コアを連結する磁気光学材
料からなる磁性薄膜とによって閉磁路が形成されている
磁気ヘッドであって、前記第1の磁気コアの前記第2の
磁気コアに対面する面、あるいは前記第2の磁気コアの
前記第1の磁気コアに対面する面の少なくとも一方に磁
気遮蔽部材が配設されていることを特徴とする磁気ヘッ
ド。
4. A magnetic gap is provided on the side of the magnetic recording medium, and the first magnetic core and the second magnetic core face each other through the magnetic gap, and the first magnetic core and the second magnetic core face each other. A magnetic head in which a closed magnetic circuit is formed by a magnetic core and a magnetic thin film made of a magneto-optical material connecting both magnetic cores, the surface of the first magnetic core facing the second magnetic core. Alternatively, a magnetic shielding member is provided on at least one of the surfaces of the second magnetic core facing the first magnetic core.
【請求項5】 磁気遮蔽部材は、導電性材料からなるこ
とを特徴とする請求項4に記載の磁気ヘッド。
5. The magnetic head according to claim 4, wherein the magnetic shield member is made of a conductive material.
【請求項6】 磁気遮蔽部材は、超電導材料からなるこ
とを特徴とする請求項4に記載の磁気ヘッド。
6. The magnetic head according to claim 4, wherein the magnetic shield member is made of a superconducting material.
JP6242841A 1994-10-06 1994-10-06 Magnetic head Pending JPH08106664A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6242841A JPH08106664A (en) 1994-10-06 1994-10-06 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6242841A JPH08106664A (en) 1994-10-06 1994-10-06 Magnetic head

Publications (1)

Publication Number Publication Date
JPH08106664A true JPH08106664A (en) 1996-04-23

Family

ID=17095095

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6242841A Pending JPH08106664A (en) 1994-10-06 1994-10-06 Magnetic head

Country Status (1)

Country Link
JP (1) JPH08106664A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1139341A4 (en) * 1998-12-07 2005-11-16 Fujitsu Ltd INFORMATION REPRODUCING DEVICE, INFORMATION REPRODUCING HEAD HAVING THE CHIP, AND INFORMATION REPRODUCING METHOD

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1139341A4 (en) * 1998-12-07 2005-11-16 Fujitsu Ltd INFORMATION REPRODUCING DEVICE, INFORMATION REPRODUCING HEAD HAVING THE CHIP, AND INFORMATION REPRODUCING METHOD

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