JPH01199301A - magneto-optical storage device - Google Patents
magneto-optical storage deviceInfo
- Publication number
- JPH01199301A JPH01199301A JP2194888A JP2194888A JPH01199301A JP H01199301 A JPH01199301 A JP H01199301A JP 2194888 A JP2194888 A JP 2194888A JP 2194888 A JP2194888 A JP 2194888A JP H01199301 A JPH01199301 A JP H01199301A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- head
- optical
- magneto
- magnetic 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording 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
- G11B11/10—Recording 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
- G11B11/105—Recording 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
- G11B11/1055—Disposition or mounting of transducers relative to record carriers
- G11B11/1058—Flying heads
Landscapes
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は光磁気記録装置に係わり、特に磁界変調記録方
式によるオーバーライド可能な光磁気ディスク装置に関
する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magneto-optical recording device, and more particularly to a magneto-optical disk device that can be overridden using a magnetic field modulation recording method.
[従来の技術]
従来、オーバーライド可能な光磁気ディスク装置として
は、特開昭51−107121号、特開昭59−215
008号、特公昭60−48806号記載のように記録
膜への印加磁界を記録する情報に応じて変調させる方式
がある。本発明は、この磁界変調記録方式による光磁気
記録装置の改良に関するものである。[Prior Art] Conventionally, overridable magneto-optical disk devices are disclosed in Japanese Patent Application Laid-open No. 51-107121 and Japanese Patent Laid-Open No. 59-215.
There is a method, as described in No. 008 and Japanese Patent Publication No. 60-48806, in which the magnetic field applied to the recording film is modulated according to the information to be recorded. The present invention relates to an improvement of a magneto-optical recording device using this magnetic field modulation recording method.
[発明が解決しようとする課題]
従来、磁界変調記録方式によるオーバーライドの例では
、ディスク上に磁界発生用電磁コイルを設置し、変調磁
界を印加していた。両者の間隔は0.1mm〜0.4m
m程度に固定されていた。この場合、記録周波数は0.
5MHz以下であり、数M Hz程度の周波数の信号記
録を行なうことができないという問題があった。[Problems to be Solved by the Invention] Conventionally, in an example of overriding using a magnetic field modulation recording method, an electromagnetic coil for generating a magnetic field is installed on a disk, and a modulated magnetic field is applied. The distance between the two is 0.1mm to 0.4m
It was fixed at about m. In this case, the recording frequency is 0.
There was a problem in that it was not possible to record signals at a frequency of about several MHz, which was 5 MHz or less.
本発明の目的は、上記の問題点を解決し、数M Hz程
度の信号が記録可能で、磁気ディスクの長所であるオー
バーライド機能と光ディスクの長所である高密度性・大
容量の両方を兼備えた光磁気記憶装置を提供することに
ある。The purpose of the present invention is to solve the above problems, to be able to record signals of about several MHz, and to have both the override function, which is an advantage of magnetic disks, and the high density and large capacity, which are advantages of optical disks. An object of the present invention is to provide a magneto-optical storage device.
[課題を解決するための手段]
上記の目的を達成するため、本発明では記録担体を挾ん
で光ヘッドと磁気ヘッドを対向させるとともに、該磁気
ヘッドとして浮上型磁気ヘッドを用い、記録担体の基板
側から光ヘッドにより光を照射し、光磁気記録膜側から
磁気ヘッドにより記録情報に応じて極性反転あるいは強
度変調された磁界を印加することによって記録を行なう
。[Means for Solving the Problems] In order to achieve the above object, in the present invention, an optical head and a magnetic head are opposed to each other by sandwiching a record carrier, and a floating magnetic head is used as the magnetic head, and the substrate of the record carrier is Recording is performed by irradiating light with an optical head from the side and applying a magnetic field whose polarity is reversed or whose intensity is modulated according to the recording information using the magnetic head from the magneto-optical recording film side.
浮上型磁気ヘッドは、有効磁界印加領域の広い(0,2
mmX0.5mm)へラドコアと低線速度でも浮上量の
大きな(1μm以上)スライダーとからなる。さらに、
該磁気ヘッドは、コの字型の磁性体コアを非磁性のスラ
イダーに埋め込んだ構造とすることを特徴とする。The floating magnetic head has a wide effective magnetic field application area (0,2
It consists of a rad core (mm x 0.5 mm) and a slider with a large flying height (1 μm or more) even at low linear speeds. moreover,
The magnetic head is characterized by having a structure in which a U-shaped magnetic core is embedded in a non-magnetic slider.
[作用]
本発明で用いる浮上型磁気ヘッドは有効磁界印加領域が
従来の磁気ヘッドに比べてはるかに広く、例えば0.2
mmX0.5mm程度であれば、絞り込みスポットと磁
気ヘッドの位置合せが容易であり、かつ、温度変化や振
動に対しても安定である。[Function] The floating magnetic head used in the present invention has a much wider effective magnetic field application area than conventional magnetic heads, for example, 0.2
If it is about mm x 0.5 mm, it is easy to align the aperture spot and the magnetic head, and it is stable against temperature changes and vibrations.
また、その浮上量が1μm以上であれば、塵等によるい
わゆるヘッドクラッシュはほとんど発生せず、通常のオ
フィス環境下での装百使用が可能となる。しかも、この
ような有効磁界印加領域の広いヘッドコアを使用した場
合、ヘッドコア端面から10〜20μm離れた位置にお
いても磁界強度はほとんど減衰しないため、光磁気記録
膜の表面には5〜10μm程度の厚い保護膜を形成する
ことができる。また、従来の塗布型磁気ディスク等と異
なり、磁性粉を含まずに純粋に保護作用のためにのみ保
護膜をコーティングできるので、保護コードの耐久性が
極めて高く、耐環境性・信頼性を一層向上させることが
できる。Further, if the flying height is 1 μm or more, so-called head crashes due to dust or the like hardly occur, and the device can be used in a normal office environment. Moreover, when such a head core with a wide effective magnetic field application area is used, the magnetic field strength hardly attenuates even at a position 10 to 20 μm away from the end face of the head core, so the surface of the magneto-optical recording film has a thickness of about 5 to 10 μm. A protective film can be formed. In addition, unlike conventional coated magnetic disks, etc., a protective film can be coated purely for protection without containing magnetic powder, making the protective cord extremely durable and further improving environmental resistance and reliability. can be improved.
本発明の浮上型磁気ヘッドは、ヘッドコア部分のみが磁
性体であるため、インダクタンスを小さくすることが可
能である。これによって磁界反転時間が短縮され、高周
波の記録が可能となる。またへラドコア部分のコの字型
とすることにより、磁界の印加効率を向上させることが
できる。さらにスライダ一部分を非磁性材質とすること
により、絞り込みレンズアクチュエータ等から漏洩する
磁界のために光磁気記録膜に印加される実効的な磁界強
度が低下することを防ぐことができる。In the floating magnetic head of the present invention, since only the head core portion is made of a magnetic material, it is possible to reduce inductance. This shortens the magnetic field reversal time and enables high frequency recording. Further, by forming the helad core portion into a U-shape, the efficiency of applying the magnetic field can be improved. Furthermore, by making a portion of the slider from a non-magnetic material, it is possible to prevent the effective magnetic field strength applied to the magneto-optical recording film from decreasing due to the magnetic field leaking from the diaphragm lens actuator or the like.
情報の記録は、光磁気記録膜に光ヘッドによって高出力
のレーザ光を基板側から照射すると同時に、磁気ヘッド
によって記録情報に応じて極性反転あるいは強度変調さ
れた変調磁界を光磁気記録膜側から印加することで行な
う。これによって、古い信号を消去しつつ新しい信号を
重ね書きすることができる。すなわち、光記録の特徴で
ある非接触という点をほとんど損なうことなく、光ディ
スクの高密度・大容量と、磁気ディスクのオーバーライ
ド機能を兼備えた光磁気記録装置が実現できる。Information is recorded by irradiating the magneto-optical recording film with high-power laser light from the substrate side using an optical head, and at the same time, from the magneto-optical recording film side, a modulated magnetic field whose polarity is reversed or whose intensity is modulated according to the recorded information is sent by a magnetic head. This is done by applying a voltage. This allows new signals to be overwritten while erasing old signals. That is, it is possible to realize a magneto-optical recording device that has both the high density and large capacity of an optical disk and the override function of a magnetic disk, without substantially impairing the non-contact characteristic of optical recording.
[実施例コ
以下、本発明の一実施例を第1図により説明する。図に
おいて、1は回転する記録担体である光磁気ディスクで
、ディスク状の透明基板103上に、磁気光学効果をも
つ光磁気記録膜101と保護膜102を有している。例
えば、半導体レーザ2からなる光源から出射した光は、
コリメートレンズ3によって平行光束に変換され、ビー
ムスプリッタ4を介して、絞り込みレンズ5に入射する
。[Example 1] An example of the present invention will be described below with reference to FIG. In the figure, reference numeral 1 denotes a magneto-optical disk which is a rotating recording carrier, and has a magneto-optical recording film 101 having a magneto-optic effect and a protective film 102 on a disk-shaped transparent substrate 103. For example, the light emitted from the light source consisting of the semiconductor laser 2 is
The collimating lens 3 converts the light into a parallel light beam, which enters the diaphragm lens 5 via the beam splitter 4.
レンズ5により絞り込まれる光ビームはディスク基板1
03側からディスクに入射し記録膜101上ニ直ffl
約1μmの縮小スポットを形成する。絞り込みレンズ5
はディスク1の上下振れに追従して常に記録膜上に焦点
がくるように、また、ディト
スフ上の情報記録用テラツクの偏心に追従して常に所望
のトラック上に光スポットがくるように。The light beam narrowed down by the lens 5 is directed to the disk substrate 1.
It enters the disk from the 03 side and hits the recording film 101 directly ffl
A reduced spot of approximately 1 μm is formed. Aperture lens 5
The light spot follows the vertical movement of the disk 1 so that the focus is always on the recording film, and it also follows the eccentricity of the information recording terrace on the disk so that the light spot always falls on the desired track.
アクチュエータ6に取付けられている。ディスク1から
の反射光は、絞り込みレンズ5を通ってビームスプリッ
タ4によって反射され、ビームスプリッタフによって光
磁気信号検出光学系8と焦点ずれおよびトラックずれ検
出等の光点制御信号検出光学系9に導かれる。It is attached to the actuator 6. The reflected light from the disk 1 passes through the aperture lens 5, is reflected by the beam splitter 4, and is transmitted by the beam splitter to the magneto-optical signal detection optical system 8 and the light spot control signal detection optical system 9, which detects defocus and track deviation. be guided.
図中には光磁気信号検出光学系8の一例を示しである。An example of the magneto-optical signal detection optical system 8 is shown in the figure.
これはλ/2板801と偏光ビームスプリッタ803を
用いた差動信号検出方式である。This is a differential signal detection method using a λ/2 plate 801 and a polarizing beam splitter 803.
光磁気信号検出光学系8に入射した光は、λ/2板80
1、レンズ802を通過し、偏光ビームスプリッタ80
3によってs’pの各偏光成分に分離されて光検出器8
04および805にそれぞれ集光される。両光検出器に
よって電気信号に変換された信号は、差動増幅機10に
よって差動され、光磁気信号として得られる。The light incident on the magneto-optical signal detection optical system 8 passes through the λ/2 plate 80
1. Passes through lens 802 and polarizing beam splitter 80
3 into each polarization component of s'p and sent to a photodetector 8.
04 and 805, respectively. The signals converted into electrical signals by both photodetectors are differentiated by a differential amplifier 10 and obtained as a magneto-optical signal.
磁気ヘッド12は、ディスク1を挾んで光ヘッド11と
対向させて記録膜側に配置する。第1図中では説明のた
め、磁気ヘッドは実際の配置からディスク面内で90°
回転させ、かつ鳥観図として拡大図示しである。磁気ヘ
ッド12は、後述するように記録膜に磁界を印加するコ
イル部分とヘッド全体を浮上させるスライダ一部分から
構成され、ディスク回転中はディスク回転による空気圧
で浮上させる。浮上量は1μm以上(好ましくは2μm
以上)である。この程度の浮上量であれば、磁気ディス
クで問題となるような、塵等によるヘッドクラッシュは
起らず、装置の大気中での使用および媒体交換を可能と
することができる。The magnetic head 12 is placed on the recording film side, sandwiching the disk 1 and facing the optical head 11. For the sake of explanation in Figure 1, the magnetic head is 90° in the disk plane from the actual arrangement.
It is rotated and enlarged as a bird's-eye view. As will be described later, the magnetic head 12 is composed of a coil portion that applies a magnetic field to a recording film and a slider portion that levitates the entire head. During disk rotation, the magnetic head 12 is levitated by air pressure generated by the disk rotation. The flying height is 1 μm or more (preferably 2 μm)
above). With this level of flying height, head crashes caused by dust and the like, which are a problem with magnetic disks, do not occur, and the device can be used in the atmosphere and media can be exchanged.
磁気ヘッド12はまた。支持バネ13によって510g
程度の荷重でディスク1に押え付けられている。ディス
クの回転開始時および停止時には、磁気ヘッドをディス
クに接触させておくいわゆるC S S (Conta
ct 5tart 5top)方式あるいはディスク回
転数が一定になるまで磁気ヘッドをディスクから離して
おく方式いずれを用いてもかまわない、ただ、ディスク
1を交換する場合は、上記2つの方式いずれをとるにし
ても磁気ヘッド12を上下させる移動機構16が必要で
ある。The magnetic head 12 is also. 510g due to support spring 13
It is pressed against the disk 1 with a certain amount of load. When the disk starts and stops rotating, the magnetic head is kept in contact with the disk.
You can use either the ct 5tart 5top) method or the method of keeping the magnetic head away from the disk until the disk rotation speed becomes constant. However, when replacing disk 1, regardless of which of the above two methods you use, Also, a moving mechanism 16 for moving the magnetic head 12 up and down is required.
磁気ヘッド12は、さらに光ヘッド11と支持アーム1
5によって一体結合されて、光ヘッドと連動可能に構成
されており、両者間の距離を一定とすると同時に常にデ
ィスク上の光スポツト真上に磁気ヘッドを設置させる。The magnetic head 12 further includes an optical head 11 and a support arm 1.
5, and is configured to be able to operate in conjunction with the optical head, so that the distance between them is constant and at the same time the magnetic head is always placed directly above the optical spot on the disk.
必ずしも、両者を図のように一体化する必要はないが、
一体結合しない場合には記録位置をディスク半径方向に
移動させる場合、両者間の距離を一定とする手段および
光スポツト真上に磁気ヘッドを設置するための磁気ヘッ
ド移動手段が必要となる。It is not necessarily necessary to integrate the two as shown in the diagram, but
If the recording position is not integrally coupled and the recording position is moved in the radial direction of the disk, means for keeping the distance between the two constant and magnetic head moving means for placing the magnetic head directly above the optical spot are required.
光ヘッド11は、例えばリニアモータあるいはステップ
モータ等によってディスク半径方向に移動させる。The optical head 11 is moved in the radial direction of the disk by, for example, a linear motor or a step motor.
第2図に、情報の記録方法を示す。情報をv!録するに
は、半導体レーザ2を第2図(b)のように高出力で連
続発光させてディスク1上の光磁気記録膜101の温度
をキュリー温度近くに加熱し、光が照射された部分の保
磁力を低下させる。この時磁気ヘッド12を、磁気ヘッ
ド駆動回路14で駆動し、記録情報(第2図(a))に
応じて極性反転させた変調磁場(第2図(C))を光磁
気記録膜101に印加し、情報の記録を行なう。記録状
態を第2図(d)に示す。なお、ディスク内外周やレー
ザ出力変動によらず、記録条件を一定にするために印加
磁場強度を変化させる必要がある場合は、極性反転だけ
でなく1強度変調あるいは磁場に、直流的なバイアス成
分を加える。この方式によれば、情報が記録されている
部分に新たに記録を行なっても、古い記録情報が残るこ
とはなく、オーバーライドすなわち、情報を重ね書きす
ることによって古い情報を消去することが可能となる。FIG. 2 shows a method of recording information. Information v! To record, the temperature of the magneto-optical recording film 101 on the disk 1 is heated to near the Curie temperature by continuously emitting light from the semiconductor laser 2 at high output as shown in FIG. 2(b), and the area irradiated with light is decreases the coercive force of At this time, the magnetic head 12 is driven by the magnetic head drive circuit 14, and a modulated magnetic field (FIG. 2(C)) whose polarity is reversed according to the recorded information (FIG. 2(a)) is applied to the magneto-optical recording film 101. Apply voltage and record information. The recording state is shown in FIG. 2(d). In addition, if it is necessary to change the applied magnetic field strength in order to keep the recording conditions constant regardless of changes in the inner or outer circumference of the disk or laser output, in addition to polarity reversal, one intensity modulation or a direct current bias component to the magnetic field can be applied. Add. According to this method, even if new information is recorded in the area where information is already recorded, the old recorded information will not remain, and it is possible to erase the old information by overwriting, that is, by overwriting the information. Become.
ここで、本実施例の主要構成要素である磁気ヘッドにつ
いて詳しく説明する。Here, the magnetic head, which is the main component of this embodiment, will be explained in detail.
磁気へラド12は、線速度が遅くても浮上量が大きく、
かつ有効磁場印加領域の広い浮上型磁気ヘッドを用いる
。ゴミ等によるヘッドクラッシュ防止の観点から浮上量
は1μm以上(好ましくは2μm以上)、光スポットと
磁気ヘッドの位置合わせの観点から、ヘッドコアの有効
磁場印加領域は0.1mmX0.1mm以上以上mX1
mm以下、好ましくは0.1mmX0.1mm以上、0
.2mmX0.5mm以下とする。The magnetic herad 12 has a large flying height even when the linear velocity is low,
In addition, a floating magnetic head with a wide effective magnetic field application area is used. From the perspective of preventing head crashes due to dust etc., the flying height should be 1 μm or more (preferably 2 μm or more), and from the perspective of alignment between the optical spot and the magnetic head, the effective magnetic field application area of the head core should be 0.1 mm x 0.1 mm or more m x 1
mm or less, preferably 0.1 mm x 0.1 mm or more, 0
.. The size shall be 2 mm x 0.5 mm or less.
第3図に本発明における浮上型磁気ヘッドの構造を示す
。第3図(a)は磁気ヘッドの鳥観図。FIG. 3 shows the structure of a floating magnetic head according to the present invention. FIG. 3(a) is a bird's eye view of the magnetic head.
第3図(b)はその展開図である。磁気コア301は例
えばMn−Zn等の磁性体であリコの字型をしている。FIG. 3(b) is a developed view thereof. The magnetic core 301 is made of a magnetic material such as Mn-Zn, and has a rectangular shape.
さらにこの磁気コア301は例えばセラミック等の非磁
性材質よりなるスライダー302に埋め込まれている。Furthermore, this magnetic core 301 is embedded in a slider 302 made of a non-magnetic material such as ceramic.
従来磁気ディスク等に用いられている磁気ヘッドは、磁
気コアとスライダーが一体加工であり、スライダ一部分
も磁性体であった。この磁気ヘッドをそのまま光磁気デ
ィスクに採用すると、例えば絞り込みレンズアクチュエ
ータから漏洩する磁界がスライダ一部分に集中するため
、磁気コアから発生する磁界の極性によっては両磁界が
お互いに相殺する方向に働き、記録膜に印加される実効
的な磁界強度が低下してしまう、スライダー302を非
磁性材質とすれば上記の現象は起らず、磁気コアから発
生する磁界を効率良く記録膜に印加することができる。In conventional magnetic heads used for magnetic disks and the like, a magnetic core and a slider are integrally fabricated, and a portion of the slider is also made of a magnetic material. If this magnetic head is used as is in a magneto-optical disk, for example, the magnetic field leaking from the aperture lens actuator will concentrate on a part of the slider, so depending on the polarity of the magnetic field generated from the magnetic core, both magnetic fields will work in a direction that cancels each other out, causing recording. If the slider 302 is made of a non-magnetic material, the effective magnetic field strength applied to the film is reduced, the above phenomenon does not occur, and the magnetic field generated from the magnetic core can be efficiently applied to the recording film. .
さらに、磁気ヘッド全体を磁性体とする場合に比べて磁
性体量の少ない構造とすることができるため、磁気ヘッ
ドのインダクタンスを低下させることができ、より高周
波の記録が可能となるという効果もある。Furthermore, since the structure can have a smaller amount of magnetic material than when the entire magnetic head is made of magnetic material, the inductance of the magnetic head can be lowered, making it possible to record higher frequencies. .
磁気ヘッド12はコの字型磁気コアの一端301aが絞
り込みスポット501の真上にくるように設置する。磁
力線は図に示すような分布をとるので、コの字型磁気コ
アの一端301b真下においては301aと逆向きの磁
界が発生している。これを利用すれば、コの字型磁気コ
アの両端301aおよび301bそれぞれの真下に絞り
込みスポットを配置させることにより、一方を記録スポ
ット、他方を消去スポットとして、2個の光スポットを
用いたオーバーライドを行うこともできる。The magnetic head 12 is installed so that one end 301a of the U-shaped magnetic core is directly above the narrowing spot 501. Since the lines of magnetic force have a distribution as shown in the figure, a magnetic field in the opposite direction to 301a is generated directly below one end 301b of the U-shaped magnetic core. By utilizing this, by arranging focused spots just below both ends 301a and 301b of the U-shaped magnetic core, one can be used as a recording spot and the other as an erasing spot, allowing override using two optical spots. You can also do this.
磁気コアの巻fi303はコの字型磁気コアのうち絞り
込みスポット真上にあるコアの巻かれている。これによ
り、端面301aで発生する磁界の強度を高め、磁界発
生効率を高めることができる。The winding fi303 of the magnetic core is the winding of the core directly above the narrowing spot of the U-shaped magnetic core. Thereby, the strength of the magnetic field generated at the end surface 301a can be increased, and the efficiency of magnetic field generation can be increased.
巻線303の位置がスライダー摺動面に近いほど、磁界
発生効率を高め、かつ磁気ヘッドのインダクタンスを低
下させることができる。この点から、 4スライダー
302において磁気コア303を支持する部分の厚さ(
図中dで示した部分)が機械的強度の観点から充分でな
い場合は、第4図に示すようにコの字型磁気コアの上下
両方を支持する構造とする。The closer the winding 303 is located to the slider sliding surface, the higher the magnetic field generation efficiency and the lower the inductance of the magnetic head. From this point, the thickness of the portion of the slider 302 that supports the magnetic core 303 (
If the portion indicated by d in the figure is not sufficient from the viewpoint of mechanical strength, a structure is adopted in which both the upper and lower sides of the U-shaped magnetic core are supported as shown in FIG.
以上の説明においてはスライダーとして、いわゆる2本
レールを持った構造を示したが、他の構造のスライダー
に対しても本発明は適用可能である。また磁気コアを埋
め込む位置に関しても1本実施例においては、一方のレ
ール上で空気の流出端に近い部分としであるが、2本レ
ールの中央部、あるいは流出端と流入端の中央部等いず
れの位置であっても本発明が適用可能であることは言う
までもない。In the above description, the slider has a so-called two-rail structure, but the present invention is also applicable to sliders with other structures. Regarding the position of embedding the magnetic core, in this embodiment, it is placed on one rail near the air outflow end, but it can be placed in the center of two rails, or in the center between the outflow end and the inflow end. It goes without saying that the present invention is applicable even in the position of .
[発明の効果]
以上説明したように1本発明によれば、磁界発生効率を
向上させるとともに、磁気コイルのインダクタンスを低
下させることができるため、低電流で高速の磁界変調記
録が可能となる。[Effects of the Invention] As explained above, according to the present invention, the magnetic field generation efficiency can be improved and the inductance of the magnetic coil can be reduced, so that high-speed magnetic field modulation recording can be performed with low current.
第1図は本発明における装置の全体構成を示す図、第2
図は磁界変調記録の記録原理を示す図、の他の実施例を
示す図である。
1・・・ディスク、2・・・半導体レーザ、3・・コリ
メートレンズ、4・・・ビームスプリッタ、5・・・絞
り込みレンズ、8・・・光磁気信号検出系、9・・・光
点側(卸信号検出系、11・・・光ヘッド、12・・・
磁気ヘッド。
系1TiJ
ノdノコjと≧m九訂銖ボ
ツー22纜書[L
ノー、?? テ2スクガー帖(
猶 2 日
(tl)言乙(珠嬉4Y
グーξネ4也−)/j
第 4 望
グθ2
手 続 補 正 書FIG. 1 is a diagram showing the overall configuration of the device according to the present invention, and FIG.
The figure is a diagram showing another embodiment of the diagram showing the recording principle of magnetic field modulation recording. DESCRIPTION OF SYMBOLS 1... Disk, 2... Semiconductor laser, 3... Collimating lens, 4... Beam splitter, 5... Stopping lens, 8... Magneto-optical signal detection system, 9... Light spot side (Wholesale signal detection system, 11...optical head, 12...
magnetic head. System 1 TiJ Nod Noko j and ≧m 9th edition Botu 22 manuscript [L No,? ? Te 2 Skuga cho (Yu 2nd (tl) Word Otsu (Jurei 4Y Gu ξne 4ya-) /j 4th Mogu θ2 Procedure Amendment Book
Claims (1)
るいは強度変調された磁界を記録担体上の光磁気記録膜
に印加するとともに、該記録担体を挾んで該浮上型磁気
ヘッドと対向させた光ヘッドから高出力のレーザ光を連
続照射することによって、情報の記録を行なう光磁気記
憶装置において、上記磁気ヘッドは、該記録担体に磁界
を印加する磁気コアと該磁気ヘッドを浮上させるスライ
ダーとが異なる材質よりなることを特徴とする光磁気記
憶装置。 2、上記磁気コアが磁性体であり、上記スライダーが非
磁性体であることを特徴とする特許請求の範囲第1項記
載の光磁気記憶装置。 3、上記磁気コアがコの字型であり、該コアの一端を絞
り込みレーザスポットの直上に配置することによって該
記録担体に磁界を印加することを特徴とする特許請求の
範囲第1項記載の光磁気記憶装置。 4、上記磁気コアの巻線は上記記録担体に磁界を印加す
る側のコア端に施され、上記スライダーの摺動面に近接
して配置されていることを特徴とする特許請求の範囲第
1項記載の光磁気記憶装置。[Claims] 1. A magnetic field whose polarity is reversed or whose intensity is modulated according to recorded information is applied to the magneto-optical recording film on the record carrier by a floating magnetic head, and the floating magnetic head is placed between the recording carrier and the magneto-optical recording film. In a magneto-optical storage device that records information by continuously irradiating high-output laser light from an optical head facing the recording medium, the magnetic head includes a magnetic core that applies a magnetic field to the recording carrier and a magnetic head that connects the magnetic core to the recording medium. A magneto-optical storage device characterized in that a floating slider is made of different materials. 2. The magneto-optical storage device according to claim 1, wherein the magnetic core is a magnetic material and the slider is a non-magnetic material. 3. The magnetic core according to claim 1, wherein the magnetic core is U-shaped, and the magnetic field is applied to the record carrier by narrowing one end of the core and placing it directly above the laser spot. Magneto-optical storage device. 4. Claim 1, characterized in that the winding of the magnetic core is provided at the end of the core on the side that applies a magnetic field to the record carrier, and is disposed close to the sliding surface of the slider. Magneto-optical storage device as described in .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63021948A JP2685471B2 (en) | 1988-02-03 | 1988-02-03 | Magneto-optical storage device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63021948A JP2685471B2 (en) | 1988-02-03 | 1988-02-03 | Magneto-optical storage device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01199301A true JPH01199301A (en) | 1989-08-10 |
| JP2685471B2 JP2685471B2 (en) | 1997-12-03 |
Family
ID=12069283
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63021948A Expired - Fee Related JP2685471B2 (en) | 1988-02-03 | 1988-02-03 | Magneto-optical storage device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2685471B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5386400A (en) * | 1990-01-19 | 1995-01-31 | Sharp Kabushiki Kaisha | Magneto-optical head device having a lubricated member |
| EP0438315B1 (en) * | 1990-01-19 | 1997-06-18 | Sharp Kabushiki Kaisha | Magneto-optical recording device |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58118026A (en) * | 1981-12-29 | 1983-07-13 | Fujitsu Ltd | Optical magnetic head |
| JPS58173023U (en) * | 1982-05-17 | 1983-11-18 | 富士電気化学株式会社 | Narrow track composite digital magnetic head |
| JPS6139251A (en) * | 1984-07-27 | 1986-02-25 | Sony Corp | Magnetic recording optical reproducing device |
| JPS632216U (en) * | 1986-06-19 | 1988-01-08 |
-
1988
- 1988-02-03 JP JP63021948A patent/JP2685471B2/en not_active Expired - Fee Related
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58118026A (en) * | 1981-12-29 | 1983-07-13 | Fujitsu Ltd | Optical magnetic head |
| JPS58173023U (en) * | 1982-05-17 | 1983-11-18 | 富士電気化学株式会社 | Narrow track composite digital magnetic head |
| JPS6139251A (en) * | 1984-07-27 | 1986-02-25 | Sony Corp | Magnetic recording optical reproducing device |
| JPS632216U (en) * | 1986-06-19 | 1988-01-08 |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5386400A (en) * | 1990-01-19 | 1995-01-31 | Sharp Kabushiki Kaisha | Magneto-optical head device having a lubricated member |
| EP0438315B1 (en) * | 1990-01-19 | 1997-06-18 | Sharp Kabushiki Kaisha | Magneto-optical recording device |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2685471B2 (en) | 1997-12-03 |
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