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JPH03263639A - Magneto-optical recording device - Google Patents

Magneto-optical recording device

Info

Publication number
JPH03263639A
JPH03263639A JP6389190A JP6389190A JPH03263639A JP H03263639 A JPH03263639 A JP H03263639A JP 6389190 A JP6389190 A JP 6389190A JP 6389190 A JP6389190 A JP 6389190A JP H03263639 A JPH03263639 A JP H03263639A
Authority
JP
Japan
Prior art keywords
magnetic field
magneto
magnetic
optical recording
optical
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
Application number
JP6389190A
Other languages
Japanese (ja)
Other versions
JP2791171B2 (en
Inventor
Kazunori Ishii
和慶 石井
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP6389190A priority Critical patent/JP2791171B2/en
Publication of JPH03263639A publication Critical patent/JPH03263639A/en
Application granted granted Critical
Publication of JP2791171B2 publication Critical patent/JP2791171B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a magneto-optical recording device, which can use both of a magneto-optical recording medium for optical modulation recording and a magneto-optical recording medium for magnetic field modulation recording where direct overwriting can be executed, without making the scale of the device large by making the constitution of the device that a magnetic field is impressed on the magneto-optical recording medium through a floating slider. CONSTITUTION:A magnetic head H which modulates a magnetic field is pro vided on the floating slider 5 and a bias magnet 7 which generates the steady magnetic field is fixedly arranged to the upper part of the slider 5. At an action time, the slider 5 is lifted to the extent of 0.1-0.9mm and held. Besides, the magnetic field generated by the magnet 7 is impressed on the magneto-optical recording medium through the slider 5. In such a case, since a large moving mechanism is not used for the head H, an error between the position of the head H by the elevating and lowering action of the slider 5 and the position of a laser spot by an optical head 1 is kept to be <=0.05mm. Thus, both of the medium for optical modulation system recording and the medium for mag netic field system recording where the direct overwriting can be executed can be used.

Description

【発明の詳細な説明】 [産業上の利用分野コ 本発明は磁界変調方式記録と光変調方式記録の兼用か可
能な光磁気記録装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magneto-optical recording device capable of both magnetic field modulation recording and optical modulation recording.

[従来の技術] 従来、光磁気記録装置としては、光ビームの強度を情報
信号によって変調し、光磁気記録媒体である光磁気ディ
スクに照射しつつ、照射部分に外部磁界を印加して情報
信号の記録を行なう方式、いわゆる光変調方式記録か知
られており実用化がなされている。この方式の記録原理
について第3図により説明する。記録する前の初期状態
において光磁気ディスク100中の磁性膜100bの磁
化は一様に下向きになっているものとする。ここで情報
信号によって光ビームを発生するレーザ光源101のオ
ン・オフを制御する。102はレーザ光源を点灯させる
トラオフ回路である。レーザ光は、光学系103によっ
て磁性膜100b上に集光される。レーザ光か照射され
るとレーザ光の照射された部分(スポット)の温度は上
昇し、キュリー温度以上になると、磁化反転か容易にな
る。一方、バイアスマクネット104は、定電流源10
5より直流定電流か供給されディスク面に対して上向の
定常磁界Bを発生する。そこで磁性膜100b上にはレ
ーザ光の照射された部分のみ磁化か反転して上向きとな
り、レーザ光照射部分を通過し、温度か下降することに
より磁化か保存されるのである。レーザ光のオン・オフ
により、磁性膜100b中にはレーザスポットとほぼ同
し大きさ(lILm程度)の磁化領域のパターンによっ
て情報信号か記録されるのである。ここで図中1008
は磁性膜100bを保持する保護膜、100Cはガラス
またはプラスチックの基板である。
[Prior Art] Conventionally, a magneto-optical recording device modulates the intensity of a light beam with an information signal and irradiates it onto a magneto-optical disk, which is a magneto-optical recording medium, while applying an external magnetic field to the irradiated portion to generate an information signal. A recording method, so-called optical modulation recording, is known and has been put into practical use. The recording principle of this method will be explained with reference to FIG. It is assumed that in the initial state before recording, the magnetization of the magnetic film 100b in the magneto-optical disk 100 is uniformly directed downward. Here, the on/off of the laser light source 101 that generates the light beam is controlled by the information signal. 102 is a turn-off circuit that turns on the laser light source. The laser beam is focused onto the magnetic film 100b by the optical system 103. When a laser beam is irradiated, the temperature of the area (spot) irradiated with the laser beam increases, and when the temperature reaches the Curie temperature or higher, magnetization reversal becomes easy. On the other hand, the bias magnet 104 is connected to the constant current source 10
A constant DC current is supplied from 5 to generate an upward steady magnetic field B against the disk surface. Therefore, the magnetization of only the portion of the magnetic film 100b that is irradiated with the laser beam is reversed so that it points upward, and as the magnet passes through the portion of the laser beam that is irradiated and the temperature decreases, the magnetization is preserved. By turning on and off the laser beam, an information signal is recorded in the magnetic film 100b by a pattern of magnetized regions approximately the same size as the laser spot (about 1ILm). Here 1008 in the figure
100C is a protective film that holds the magnetic film 100b, and 100C is a glass or plastic substrate.

また記録された情報信号の再生は磁化の方向の変化て磁
性膜100bに記録された情報信号を磁気カー効果とよ
ばれる光と磁気の相互作用を利用し一定強度のレーザ光
を入射し、反射レーザ光の偏光面の回転を検出すること
によって行なうのである。
In addition, to reproduce the recorded information signal, the information signal recorded on the magnetic film 100b is reflected by changing the direction of magnetization by injecting a laser beam of a certain intensity using the interaction between light and magnetism called the magnetic Kerr effect. This is done by detecting the rotation of the polarization plane of the laser beam.

磁気カー効果とは、直線偏光のレーザ光を垂直磁化膜に
入射させると、反射光の偏光面が磁化の向きに従って、
左または右に回転する現象である。この回転を検光子に
よって光量変化に変換して情報信号の再生を行なう。
The magnetic Kerr effect is when linearly polarized laser light is incident on a perpendicularly magnetized film, the polarization plane of the reflected light changes according to the direction of magnetization.
This is a phenomenon of rotation to the left or right. This rotation is converted into a change in light amount by an analyzer to reproduce the information signal.

この方式では記録された情報信号の内容を書き換える際
にはバイアスマグネット104の発生磁界の向きを逆(
下向き)として、レーザ光を変調せずに連続照射して、
磁性膜100bの磁化の向きを一様に下向きにそろえる
いわゆる消去を行なった後に、前述した手順て情報信号
を記録するのである。
In this method, when rewriting the contents of the recorded information signal, the direction of the magnetic field generated by the bias magnet 104 is reversed (
(downward), the laser beam is continuously irradiated without modulation,
After so-called erasing is performed to uniformly align the direction of magnetization of the magnetic film 100b downward, an information signal is recorded using the procedure described above.

つまり、実用化されている光変調方式記録は、情報信号
の書き換えの際には必ず元の信号を消去することか必要
であり、新たな情報信号を元の情報信号の上から直接重
ね書きばてきないのである。
In other words, in the optical modulation recording system that is in practical use, it is necessary to erase the original signal when rewriting the information signal, and it is necessary to directly overwrite the new information signal on top of the original information signal. I can't.

これに対して、最近磁界変調方式記録により情報信号の
直接重ね書きか可能な装置か提案されている。(例えば
Japahese Journal of AppIl
ed Physics、Vol、26(1987)Su
pplement 2B−4゜“旧gh 5peed 
Overwritable Magneto−Opti
cRecovding”)この方式の記録原理について
、第4図により説明する。レーザ光源101は定電流源
106により供給される直流電流により、連続点灯され
るレーザ光は光学系103により磁性ill 100b
上に集光される。レーザ光の照射された部分(スポット
)の温度は、上昇しキュリー温度以上となると磁化反転
か容易になる。一方浮上スライダー107上には磁気ヘ
ット108か設けられ、ディスク100の表面との間に
1101L以下のスペースを保ちつつ、浮上走行してい
る。
In response to this, recently a device has been proposed that allows direct overwriting of information signals using magnetic field modulation recording. (For example, Japanese Journal of AppIl
ed Physics, Vol. 26 (1987) Su
pplement 2B-4゜“old gh 5peed
Overwritable Magneto-Opti
The recording principle of this method will be explained with reference to FIG.
The light is focused on the top. When the temperature of the portion (spot) irradiated with the laser beam increases and reaches the Curie temperature or higher, magnetization reversal becomes easy. On the other hand, a magnetic head 108 is provided on the floating slider 107, and flies while maintaining a space of 1101L or less between it and the surface of the disk 100.

しかし浮上スライダーかディスク表面に接触したり、こ
みを巻き込むことにより磁性膜100bか損傷を受ける
こεを防ぐために、フィラーを混入するなどした特殊な
保護l1100aかディスク100上に設けられており
、前述の光変調方式記録に用いられているディスクの保
護膜と比較し、耐久性にすくれたものとなっている6磁
気ヘット1.08は磁気へットトライッ回路109より
電流4#、粕を受け、情報信号に応じて発生磁界の方向
か反転される。高速度での情報信号記録においては磁気
ヘットを小型化し、ディスクに十分に接近させる必要か
あるため、磁界変調方式の記録は前述の光変調方式とは
異り、磁気ヘットを浮上スクイター上に設ける#戒か望
ましいのである。
However, in order to prevent the magnetic film 100b from being damaged by the flying slider coming into contact with the disk surface or by getting dust involved, a special protection l1100a containing filler or the like is provided on the disk 100. The 6 magnetic heads 1.08, which are more durable than the disk protective film used for optical modulation recording, receive a current of 4 # and lees from the magnetic head try circuit 109. The direction of the generated magnetic field is reversed depending on the information signal. To record information signals at high speeds, it is necessary to downsize the magnetic head and bring it close enough to the disk, so unlike the optical modulation method described above, magnetic field modulation recording requires the magnetic head to be placed on a floating squiter. #Precepts are desirable.

磁性膜100b中にはレーザ光の照射位置のみ温度か上
昇し、磁気ヘット108の発生する磁界の向きと同じ向
きの磁化か形成され、ディスク100の回転により、レ
ーザ光の照射位置を通過後は急激に温度か低下し、磁化
か保存されるのである。このように磁界の反転により磁
性膜】00b中には、レーザスポットと同し大きさ(1
gm程度)の磁化領域のパターンにより情報信号か記録
されるのである。この方式では情報信号の内容を書き換
える際に、磁化の向きを一度一様にそろえる消去動作は
不要てあり、上記の動作を繰り返すことにより何度でも
直接重ね書きが可能である。また情報信号の再生につい
ては前述の光変調方式とまったく同様である。
In the magnetic film 100b, the temperature rises only at the laser beam irradiation position, and magnetization is formed in the same direction as the magnetic field generated by the magnetic head 108, and as the disk 100 rotates, after passing the laser beam irradiation position, The temperature drops rapidly and the magnetization is preserved. In this way, due to the reversal of the magnetic field, the magnetic film 00b has the same size as the laser spot (1
An information signal is recorded by the pattern of the magnetized region (about 100 gm). In this method, when rewriting the contents of the information signal, there is no need for an erasing operation to uniformly align the direction of magnetization once, and by repeating the above operation, direct overwriting is possible any number of times. Furthermore, the reproduction of the information signal is exactly the same as the optical modulation method described above.

このように、実用化されている情報信号の直接重ね書き
はできない光変調方式の光磁気記録装置と、情報信号の
直接重ね書きを目的として提案された磁界変調方式の光
磁気記録装置とは、用いる光磁気記録媒体であるディス
クの保護膜、磁界印加手段の構成か異っており、全く互
換性の無いものとなっている。特に、磁界変調方式の磁
気ヘッドの発生する有効磁界範囲は直径O12璽■と小
さく、照射されるレーザスポット位置との間で0.05
mm程度の精密位置決めか必要である。そのため大型の
光変調方式用バイアスマグネットと小型の磁界変調用磁
気ヘットの両方を別個に備え、それらの位置を用いるデ
ィスクの種類によって機械的に入れ替えて使用するとい
った場合には、大きな移動機構、特にディスク面に対し
水平面内ての移動機構ては上述したレーザスポットと磁
界変調方式の磁気ヘッドの0.05mmの位置精度は保
証てきない。さらにこのように光変調方式用バイアスマ
グネットと磁界変調用磁気ヘッドとを別個に備えた場合
には、装置全体が大型化するという問題点がある。
In this way, there are optical modulation type magneto-optical recording devices that are in practical use that cannot directly overwrite information signals, and magnetic field modulation type magneto-optical recording devices that have been proposed for the purpose of direct overwriting of information signals. The protective film of the disk, which is the magneto-optical recording medium used, and the structure of the magnetic field applying means are different, making them completely incompatible. In particular, the effective magnetic field range generated by the magnetic field modulation type magnetic head is as small as a diameter of 0.01 mm, and the range of the effective magnetic field generated is 0.05 mm between the irradiated laser spot position and the irradiated laser spot position.
Precise positioning on the order of mm is required. Therefore, if both a large bias magnet for optical modulation and a small magnetic head for magnetic field modulation are separately provided and their positions are mechanically replaced depending on the type of disk used, it is necessary to use a large moving mechanism, especially The positional accuracy of 0.05 mm between the laser spot and the magnetic head of the magnetic field modulation method described above cannot be guaranteed with respect to the moving mechanism in the horizontal plane with respect to the disk surface. Furthermore, when the bias magnet for optical modulation method and the magnetic head for magnetic field modulation are separately provided in this way, there is a problem that the entire device becomes larger.

[発明の目的コ 本発明は上記事情にもとづいてなされたちのて、装置を
大型化することなく光変調記録用の光磁気記録媒体と直
接重ね書きの可能な磁界変調記録用の光磁気記録媒体の
両方か使用可能な光磁気記録装置を提供しようとするも
のである。
[Object of the Invention] The present invention was made based on the above circumstances, and provides a magneto-optical recording medium for magnetic field modulation recording that can be directly overwritten with a magneto-optical recording medium for optical modulation recording without increasing the size of the device. The aim is to provide a magneto-optical recording device that can be used for both.

[課題を解決するための手段] 本発明による光磁気記録装置は、従来の磁界変調方式記
録装置と同様に、浮上スライダー上に磁界変調用の磁気
ヘットか設けられると共に、浮上スライダーの近傍にバ
イアスマクネットを配置し、磁界変調方式記録時には従
来の磁界変調方式記録装置と同様に動作し、また、光変
調方式記録時には、浮上スライダーをバイアスマクネッ
トに接近させ、バイアスマクネットを動作させることに
より、浮上スライダーを貫いて磁界を光磁気記録媒体に
印加するよう構成し、両方式の光磁気記録媒体の使用を
可能とするものである。
[Means for Solving the Problems] The magneto-optical recording device according to the present invention, like the conventional magnetic field modulation type recording device, has a magnetic head for magnetic field modulation on the floating slider, and also has a bias near the floating slider. When recording using a magnetic field modulation method, the magnetic field modulation method recording device operates in the same way as a conventional magnetic field modulation method recording device, and when recording using an optical modulation method, the floating slider is brought close to the bias mucket and the bias mucket is operated. , the magnetic field is applied to the magneto-optical recording medium through the floating slider, thereby making it possible to use both types of magneto-optical recording media.

[実施例〕 以下第1図(a)、(b)により本発明による光磁気記
録装置の動作についた説明する。
[Example] The operation of the magneto-optical recording apparatus according to the present invention will be explained below with reference to FIGS. 1(a) and 1(b).

(a)は磁界変調方式による情報信号記録を行なう場合
の動作、(b)は光変調方式による情報信号記録を行な
う場合の動作を示す。lはレーザ光源、2はレーザ光源
を点灯させるトライツ回路である。レーザ光は光学系3
によって光磁気ディスク4中の磁性膜4b上に集光され
る。4aは磁性膜4bを保護する保護膜、4cはガラス
またはプラスチックの基板である。浮上スライダー5に
は磁芯C2および磁気ヘットHが設けられている。磁芯
C2は上面、下面か浮上スライダーの上、下に露出する
ように設けられるものとし、6は磁気ヘットHを駆動す
るトライフ回路である。本実施例ては第2図に見取り図
て示すようにフェライトなとの強磁性体より威る円柱形
の磁芯C2の下面(ディスクと対向する側の面)に円形
の溝を加工し、溝内に巻線Wを設は磁界変調用の磁気ヘ
ットHとする構成とするか、磁芯C2と磁気ヘットHと
を各別々に作製してもよい。バイアスマクネット7は磁
芯C1と巻線WBより戒り、浮上スライダー5の近傍の
上方に固定配置される。9はバイアスマクネットを駆動
する定電流源である浮上スライダ−5はアーム8により
支持され、図示しない昇降手段により、ディスク表面と
の間に10gm以下の間隔を保って浮上走行するか、ま
たはディスクの上方0.1〜Q、9mmの間隔を保って
保持することが可能である。
(a) shows the operation when recording an information signal using the magnetic field modulation method, and (b) shows the operation when recording the information signal using the optical modulation method. 1 is a laser light source, and 2 is a TRIZ circuit for lighting the laser light source. Laser light is optical system 3
The light is focused onto the magnetic film 4b in the magneto-optical disk 4. 4a is a protective film that protects the magnetic film 4b, and 4c is a glass or plastic substrate. The floating slider 5 is provided with a magnetic core C2 and a magnetic head H. The magnetic core C2 is provided so as to be exposed on the upper or lower surface of the floating slider, and 6 is a trife circuit for driving the magnetic head H. For example, as shown schematically in FIG. 2, a circular groove is machined on the lower surface (the surface facing the disk) of the cylindrical magnetic core C2, which is more powerful than a ferromagnetic material such as ferrite. The winding W may be provided inside the magnetic head H for magnetic field modulation, or the magnetic core C2 and the magnetic head H may be manufactured separately. The bias magnet 7 is fixedly disposed near and above the floating slider 5, separated from the magnetic core C1 and the winding WB. The floating slider 5, in which 9 is a constant current source for driving a bias magnet, is supported by an arm 8, and is floated and travels with a distance of 10 gm or less between the disk surface and the disk surface by means of an elevating means (not shown). It is possible to maintain a distance of 0.1 to Q, 9 mm above the .

磁界変調方式の記録を行なう場合、!$1図(a)に示
すように浮上スライダー5はディスク4の表面上を浮上
走行する。ディスク4は磁界変調方式用のディスクであ
りディスク表面には磁性膜4bを浮上スライダ−5の接
触による損傷から防ぐために十分な強度、潤滑特性等を
持つ保護膜4aか形成されている。
When recording using magnetic field modulation method,! $1 As shown in FIG. 1(a), the floating slider 5 flies above the surface of the disk 4. The disk 4 is a disk for a magnetic field modulation system, and a protective film 4a having sufficient strength, lubricating properties, etc. is formed on the surface of the disk to prevent the magnetic film 4b from being damaged by contact with the flying slider 5.

レーザー光源lは制御回路10よりの制御信号によって
情報信号の内容とは無関係に、レーザ光源ドライブ回路
2か供給する定電流により、一定光量て発光する。レー
ザ光は光学系3によって磁性!!4b上に集光される。
The laser light source 1 emits a constant amount of light by a control signal from the control circuit 10, regardless of the content of the information signal, and by a constant current supplied from the laser light source drive circuit 2. Laser light is made magnetic by optical system 3! ! The light is focused on 4b.

また磁気ヘットHには制御回路10よりの制御信号によ
って磁気ヘットトライツ回路6から情報信号(よって変
調された電流か供給され、情報信号に応じて変化する磁
界を発生してディスク4に印加される。Bは磁気ヘッド
Hの発生する磁束を示す。このようにして従来例の磁界
変調方式記録と同様にして、情報信号の記録か行なわれ
る。この時、バイアスマクネット7には電流は供給され
ず、磁界は発生しない。また光変調方式の記録を行なう
場合には第1図(b)に示すように、浮上スライダー5
はディスク4の上方O31〜0.9mmに保持される。
Further, the magnetic head H is supplied with an information signal (and thus a modulated current) from the magnetic head trites circuit 6 in response to a control signal from the control circuit 10, and a magnetic field that changes according to the information signal is generated and applied to the disk 4. B indicates the magnetic flux generated by the magnetic head H.In this way, information signals are recorded in the same manner as in the conventional magnetic field modulation recording method.At this time, no current is supplied to the bias magnet 7. , no magnetic field is generated.Furthermore, when recording by optical modulation method, as shown in FIG. 1(b), the floating slider 5
is held at a distance of 031 to 0.9 mm above the disk 4.

この時磁芯C1と磁芯C2とは密着するように構成した
方か磁界の横方向への漏れか減り、効率かよいばかりて
なく、バイアスマグネット7の磁気的吸引力により磁芯
C2を吸引し浮上スライダー5か固定されるため、都合
かよい。
At this time, if the magnetic cores C1 and C2 are configured to be in close contact with each other, the leakage of the magnetic field in the lateral direction is reduced, which not only improves efficiency, but also attracts the magnetic core C2 by the magnetic attraction force of the bias magnet 7. This is convenient because the floating slider 5 is fixed.

レーザ光[1は制御回路lOよりの制御信号によってレ
ーザ光源ドライブ回路2か供給する情報信号により変調
された電流により、情報信号に応じて発光をオン・オフ
する。レーザ光は光学系3によって磁性膜4b上に集光
される。
The laser light [1] turns on and off the light emission according to the information signal by a current modulated by the information signal supplied from the laser light source drive circuit 2 according to the control signal from the control circuit IO. The laser beam is focused by the optical system 3 onto the magnetic film 4b.

またバイアスマクネット7には制御回路10の制御信号
により定電流源9から一足電流が供給され、定常磁界を
発生する。また、バイアスマクネットによる定常磁界の
方向の切換はてきる。Bはバイアスマクネット7の発生
する磁束を示す。定常磁界は浮上スライダー5上の磁芯
C2を磁路の一部とし、磁芯C2のディスク4と対向す
る方の面からディスク4へ印加されるため、磁界の発散
による磁界強度の減衰を最小限にとどめ十分な磁界をデ
ィスク4に印加することかてきる。この時磁気ヘットH
は磁界を発生しない。このようにして従来例の光変調方
式の記録と同様にして情報信号の記録か行なわれる。こ
こて、浮上スライダー5は上方に保持され、ディスク4
表面と接触することはないため、既に実−用化されてい
る保護膜の性能か不十分な光変調用ディスク4を使用す
ることか可能である。
Further, a current is supplied to the bias magnet 7 from a constant current source 9 according to a control signal from a control circuit 10 to generate a steady magnetic field. In addition, the direction of the steady magnetic field can be switched by the bias magnet. B indicates the magnetic flux generated by the bias magnet 7. The steady magnetic field uses the magnetic core C2 on the floating slider 5 as part of the magnetic path, and is applied to the disk 4 from the surface of the magnetic core C2 facing the disk 4, so that the attenuation of the magnetic field strength due to magnetic field divergence is minimized. It is possible to apply a sufficient magnetic field to the disk 4 while limiting the magnetic field. At this time, magnetic head H
does not generate a magnetic field. In this way, information signals are recorded in the same manner as in the conventional optical modulation method recording. Here, the floating slider 5 is held upward, and the disk 4
Since there is no contact with the surface, it is possible to use a light modulating disk 4 whose protective film, which has already been put into practical use, has insufficient performance.

このような構成をとれば、浮上スライダー5上の磁芯C
2をバイアスマクネットの磁芯CIの一部とみなすこと
がてきる。
With such a configuration, the magnetic core C on the floating slider 5
2 can be regarded as part of the magnetic core CI of the bias magnet.

また、バイアスマグネット使用時に磁芯C1と磁芯C2
とは完全に密着してなくても少しくらい間かおいていて
も磁界をディスク上に発生させることか可能である。
Also, when using a bias magnet, magnetic core C1 and magnetic core C2
It is possible to generate a magnetic field on the disk even if they are not in perfect contact with each other for a while.

[発明の効果コ 以上のように本発明による光磁気記録装置は、磁界変調
を行なう磁気ヘットを浮上スライダー上に設け、また、
定常磁界を発生するバイアスマクネットを浮上スライダ
ー上方に固定配置し、バイアスマクネット動作時には浮
上スライダーを上方に0.1〜0.9mm程度持ち上げ
保持し、バイアスマクネットの発生磁界は浮上スライダ
ーを貫いて光磁気記録媒体に印加されるよう構成し、磁
界変調用磁気ヘットに対する大きな移動機構を用いない
のて、浮上スライダーの昇降動作による磁界変調用磁気
ヘットと光ヘットによるレーザスポット位置の誤差は0
.05mm以下に保たれる。従って既に実用化されてい
る光変調方式記録用の媒体と直接重ね書きの可能な磁界
変調方式記録用の媒体との両方か使用可能である。
[Effects of the Invention] As described above, the magneto-optical recording device according to the present invention includes a magnetic head for modulating a magnetic field provided on a flying slider, and
A bias macnet that generates a steady magnetic field is fixedly placed above the floating slider, and when the bias macnet is in operation, the levitating slider is lifted and held upward by about 0.1 to 0.9 mm, and the magnetic field generated by the bias macnet penetrates the floating slider. Since no large moving mechanism is used for the magnetic head for magnetic field modulation, the error in the position of the laser spot due to the vertical movement of the floating slider between the magnetic head for magnetic field modulation and the optical head is zero.
.. It is kept below 0.05mm. Therefore, it is possible to use both optical modulation recording media that have already been put into practical use and magnetic field modulation recording media that can be directly overwritten.

さらに、バイアスマクネットの磁芯の一部を浮上スライ
ダー上に設けることにより、ハイアスマクネットの発生
する磁界を効率よく媒体に印加することか可能となるば
かりてなく、バイアスマクネットの磁界的吸引力て浮上
スライダーを固定位置決めすることか可能である。
Furthermore, by providing a part of the magnetic core of the bias mucknet on the floating slider, it is not only possible to efficiently apply the magnetic field generated by the high ass mcnet to the medium, but also the magnetic field attraction of the bias mcnet It is possible to fix the position of the floating slider by force.

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

第1図(a)、(b)は本発明による光磁気記録装置の
動作を説明する図、第2図は本発明による光磁気記録装
置の磁芯C2および磁気ヘットの見取り図、第3図は従
来の光変調方式の記録装置の動作を説明する図、第4図
は従来の磁界変調方式の記録装置の動作を説明する図で
ある。 l・・・レーザ光源 2・・・レーザ光源トライヲ回路 4・・・ディスク 5・・・浮上スライダー 6・・・磁気ヘッドトライツ回路 7・・・バイアスマクネット 9・・・定電流源 O・・・制御回路 H・・・磁気ヘット C2・・・磁芯 第3図
FIGS. 1(a) and (b) are diagrams explaining the operation of the magneto-optical recording device according to the present invention, FIG. 2 is a sketch of the magnetic core C2 and the magnetic head of the magneto-optical recording device according to the present invention, and FIG. FIG. 4 is a diagram illustrating the operation of a conventional optical modulation type recording apparatus, and FIG. 4 is a diagram illustrating the operation of a conventional magnetic field modulation type recording apparatus. l... Laser light source 2... Laser light source try circuit 4... Disk 5... Flying slider 6... Magnetic head try circuit 7... Bias magnet 9... Constant current source O...・Control circuit H...Magnetic head C2...Magnetic core Figure 3

Claims (3)

【特許請求の範囲】[Claims] (1)光磁気記録媒体に対して光ビームを照射しつつ磁
界を印加することにより情報信号の記録又は消去を行な
う光磁気記録装置において、情報信号に応じて変調され
た磁界を発生する第1の磁界発生手段と、情報信号の内
容によらず定常的な磁界を発生する第2の磁界発生手段
とを有し、該第1の磁界発生手段は、浮上スライダー上
に設けられ、該第2の磁界発生手段は浮上スライダーの
近傍に配置され、該第2の磁界発生手段の発生する定常
的な磁界は、該浮上スライダーを貫いて該光磁気記録媒
体に印加されるようになされたことを特徴とする光磁気
記録装置。
(1) In a magneto-optical recording device that records or erases information signals by applying a magnetic field while irradiating a light beam to a magneto-optical recording medium, a first and a second magnetic field generating means that generates a steady magnetic field regardless of the content of the information signal, the first magnetic field generating means is provided on the floating slider, and the second magnetic field generating means is provided on the floating slider. The second magnetic field generating means is arranged near the floating slider, and the steady magnetic field generated by the second magnetic field generating means is applied to the magneto-optical recording medium through the floating slider. Features of magneto-optical recording device.
(2)前記第2の磁界発生手段の磁芯の少なくとも一部
が浮上スライダー上に設けられることを特徴とする特許
請求の範囲第1項記載の光磁気記録装置。
(2) The magneto-optical recording device according to claim 1, wherein at least a part of the magnetic core of the second magnetic field generating means is provided on a floating slider.
(3)前記第2の磁界発生手段の動作時において該第2
の磁界発生手段と浮上スライダー上に設けられた磁芯と
の間の磁気的吸引力により該浮上スライダーが固定され
ることを特徴とする特許請求の範囲第2項記載の光磁気
記録装置。
(3) When the second magnetic field generating means operates, the second magnetic field generating means
3. The magneto-optical recording device according to claim 2, wherein the floating slider is fixed by a magnetic attraction force between the magnetic field generating means and a magnetic core provided on the floating slider.
JP6389190A 1990-03-13 1990-03-13 Magneto-optical recording device Expired - Fee Related JP2791171B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6389190A JP2791171B2 (en) 1990-03-13 1990-03-13 Magneto-optical recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6389190A JP2791171B2 (en) 1990-03-13 1990-03-13 Magneto-optical recording device

Publications (2)

Publication Number Publication Date
JPH03263639A true JPH03263639A (en) 1991-11-25
JP2791171B2 JP2791171B2 (en) 1998-08-27

Family

ID=13242374

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6389190A Expired - Fee Related JP2791171B2 (en) 1990-03-13 1990-03-13 Magneto-optical recording device

Country Status (1)

Country Link
JP (1) JP2791171B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04121847A (en) * 1990-09-11 1992-04-22 Matsushita Electric Ind Co Ltd magneto-optical disk device
US5408455A (en) * 1992-04-08 1995-04-18 Asahi Kogaku Kogyo Kabushiki Kaisha Control device for head unit having optical head and multiple magnetic heads
US7446392B2 (en) 1996-07-16 2008-11-04 Semiconductor Energy Laboratory Co., Ltd. Electronic device and method for manufacturing the same

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04121847A (en) * 1990-09-11 1992-04-22 Matsushita Electric Ind Co Ltd magneto-optical disk device
US5408455A (en) * 1992-04-08 1995-04-18 Asahi Kogaku Kogyo Kabushiki Kaisha Control device for head unit having optical head and multiple magnetic heads
US5513159A (en) * 1992-04-08 1996-04-30 Asahi Kogaku Kogyo Kabushiki Kaisha Device for selecting magnetic head to be operated together with an optical head
US5592447A (en) * 1992-04-08 1997-01-07 Asahi Kogaku Kogyo Kabushiki Kaisha Control device for head unit having optical head and multiple magnetic heads
US7446392B2 (en) 1996-07-16 2008-11-04 Semiconductor Energy Laboratory Co., Ltd. Electronic device and method for manufacturing the same

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