JPS59180802A - Optical magnetic recording and reproducing device - Google Patents

Optical magnetic recording and reproducing device

Info

Publication number
JPS59180802A
JPS59180802A JP5367983A JP5367983A JPS59180802A JP S59180802 A JPS59180802 A JP S59180802A JP 5367983 A JP5367983 A JP 5367983A JP 5367983 A JP5367983 A JP 5367983A JP S59180802 A JPS59180802 A JP S59180802A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic field
disk
magnetic pole
recording
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
JP5367983A
Other languages
Japanese (ja)
Inventor
Yasuo Sawada
康雄 沢田
Masaaki Nomura
正明 野村
Hiroyuki Okamoto
弘之 岡本
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP5367983A priority Critical patent/JPS59180802A/en
Publication of JPS59180802A publication Critical patent/JPS59180802A/en
Pending legal-status Critical Current

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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
    • G11B11/10502Recording 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 characterised by the transducing operation to be executed
    • G11B11/10504Recording

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To attain the optical magnetic recording and reproduction with high accuracy by setting a flaky auxiliary magnetic pole opposite to a magnetic field generating means of an optical head part by holding a recording medium and therefore avoiding an adverse effect of the magnetic field generating means to an automatic focusing mechanism to a condensing means. CONSTITUTION:A laser beam B made incident to an objective lens 10 is focused and stopped down into a microspot on a magnetic disk 7. Thus the temperature is selectively raised up at the area irradiated by the beam B, and therefore the coercive force of the irradiated area is lowered. Both a magnetic oil 12 and an auxiliary magnetic pole 14 coact to the area S irradiated by said microspot to form a uniform magnetic field along the thickness direction. Therefore only the area S of a magnetic disk 7 is selectively magnetized toward an external magnetic field to form a microbit. The bits are formed for the 1-round course during a revolution of te disk 7. Thus the formation of bits is started to a new track obtained by giving a scan equivalent to a track performed by an optical head part H in the radius direction of the disk 7. In such a way, a microbit is formed at a recording part 7' of the disk 7 with high density and high accuracy in accordance with the input information.

Description

【発明の詳細な説明】 技術分野 本発明は磁気記録再生装置に関し、より詳細には光を書
込及び読出手段として用いる光磁気記録再生装置に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION Technical Field The present invention relates to a magnetic recording and reproducing device, and more particularly to a magneto-optical recording and reproducing device that uses light as a writing and reading means.

従来技術 従来の光磁気記録再生装置における記録ヘッド部は、通
常、第1図に示す如く構成されている。
BACKGROUND OF THE INVENTION A recording head section in a conventional magneto-optical recording/reproducing apparatus is normally constructed as shown in FIG.

第1図において、記録媒体°としての磁気ディスク1が
回転軸2に固着されモータ3により回動可能に配設され
ている。この磁気ディスク1は厚さ方向に磁気異方性を
備えた磁性薄膜で形成されている。磁気ディスク1上に
光を照射する光ヘツド部Hは、供給された光を磁気ディ
スク1上に微小スポット状に集束させる対物レンズ4と
磁気ディスク1に垂直に、すなわちその厚さ方向に沿っ
て磁界を印加する磁気コイル5及びこれらの磁気ディス
ク1に対する位置を制御するアクチュエータ6で構成さ
れている。
In FIG. 1, a magnetic disk 1 serving as a recording medium is fixed to a rotating shaft 2 and is rotatably arranged by a motor 3. As shown in FIG. The magnetic disk 1 is formed of a magnetic thin film having magnetic anisotropy in the thickness direction. The optical head H that irradiates light onto the magnetic disk 1 includes an objective lens 4 that focuses the supplied light onto the magnetic disk 1 in the shape of a minute spot, and an objective lens 4 that focuses the supplied light onto the magnetic disk 1 in the form of a minute spot, and an optical head H that is arranged perpendicularly to the magnetic disk 1, that is, along its thickness direction. It is comprised of a magnetic coil 5 that applies a magnetic field and an actuator 6 that controls the position of these with respect to the magnetic disk 1.

上述の如く構成された記録ヘッドにより実施される熱磁
気記録の1方式である光磁気記録の原理は、以下の通り
である。即ち、光源(不図示)から入力情報に従って変
調され出力された光ビームBが対物レンズ4により微小
スポラ1へ状に集束されて磁気ディスク1上に照射され
る事により、その照射部分の温度が上昇し抗磁力が低下
する。然るに、この部分には磁気コイル5による外部磁
界が磁気ディスク1の厚さ方向に付与されているため、
その方向に治ってその部分のみが選択的に磁化される。
The principle of magneto-optical recording, which is one type of thermomagnetic recording performed by the recording head configured as described above, is as follows. That is, a light beam B modulated and outputted from a light source (not shown) according to input information is focused by an objective lens 4 onto a microspora 1 and irradiated onto the magnetic disk 1, so that the temperature of the irradiated portion increases. increases and the coercive force decreases. However, since an external magnetic field is applied to this portion by the magnetic coil 5 in the thickness direction of the magnetic disk 1,
It heals in that direction and only that part is selectively magnetized.

この様にして、入力情報に応じ磁気ディスク1に微小な
磁区、即ちビットが形成され、情報が記録される。この
場合、均一なビットを形成するためには、照射される微
小スポットの大きさが一定に維持され照射部分の温度分
布が一定となることの他、この部分に付与される磁気コ
イル5による外部磁界の強さも一定となる様に各要素を
制御する必要がある。この為、例えばアクチュエータ6
にサーボ機構等を組み入れ、光ヘツド部Hを対向する磁
気ディスク1表面の微妙な上下動や凹凸に鋭敏に追従さ
せてこれら双方の対向間隔Wを高精度で一定に保持し照
射する光スポットの大きさを一定に制御するオートフォ
ーカス機構が採用されている。
In this way, minute magnetic domains, ie, bits, are formed on the magnetic disk 1 according to input information, and information is recorded. In this case, in order to form a uniform bit, in addition to maintaining the size of the irradiated minute spot constant and making the temperature distribution of the irradiated area constant, it is also necessary to It is necessary to control each element so that the strength of the magnetic field is also constant. For this reason, for example, actuator 6
A servo mechanism or the like is incorporated in the optical head H to closely follow the subtle vertical movements and irregularities on the surface of the opposing magnetic disk 1 to maintain a constant distance W between these two surfaces with high precision to create a light spot for irradiation. An autofocus mechanism is used to keep the size constant.

然るに、光ヘツド部Hの重量は対物レンズ4及び磁気コ
イル5等が装着されている為相当に重く、その結果光ヘ
ツド部Hの磁気ディスク1に対する追従性が鈍くなり対
向間隔Wを高精度で確保することは困難である。又、磁
気コイル5の形成する磁界がアクチュエータ6に内蔵さ
れたサーボ機構に悪影響を及ぼし誤差発生の一因となる
。更に、磁気コイル5には比較的大きい電流が通電され
るため、それによる発熱量も多く対物レンズ4に悪影響
が及ぶが、これによる誤差も無視できない。
However, the weight of the optical head H is quite heavy due to the attachment of the objective lens 4, magnetic coil 5, etc., and as a result, the ability of the optical head H to follow the magnetic disk 1 becomes slow, making it difficult to adjust the facing distance W with high precision. It is difficult to secure. Further, the magnetic field formed by the magnetic coil 5 has an adverse effect on the servo mechanism built into the actuator 6, contributing to the occurrence of errors. Furthermore, since a relatively large current is applied to the magnetic coil 5, the amount of heat generated is large and has an adverse effect on the objective lens 4, but the error caused by this cannot be ignored.

目  的 本発明は、以上の点に鑑みてなされたものであって、磁
界発生手段による集光手段のオートフォーカス機構に対
する悪影響を回避し高精度な光磁気記録再生処理が可能
となる光磁気記録再生処理装置を提供することを目的と
する。
Purpose The present invention has been made in view of the above points, and provides magneto-optical recording which avoids the negative influence of the magnetic field generation means on the autofocus mechanism of the focusing means and enables highly accurate magneto-optical recording and reproducing processing. The purpose is to provide a regeneration processing device.

構成 以下、本発明の構成に付いて具体的な実施例に′  基
づき説明する。第2図は、本発明が適用された光磁気記
録再往装置の記録部を示した模式図である。第2図にお
いて、記録媒体どしての円板状の磁気ディスク7が回転
軸8に固着されモータ9により回動可能に装着されてい
る。磁気ディスク7は、7bFe、GdTbFe、 T
bFeCo等の非晶質磁性体から成り、厚さ方向の垂直
磁気異方性を有している。
Configuration The configuration of the present invention will be explained below based on specific examples. FIG. 2 is a schematic diagram showing a recording section of a magneto-optical recording reciprocating device to which the present invention is applied. In FIG. 2, a disk-shaped magnetic disk 7 serving as a recording medium is fixed to a rotating shaft 8 and is mounted so as to be rotatable by a motor 9. As shown in FIG. The magnetic disk 7 is made of 7bFe, GdTbFe, T
It is made of an amorphous magnetic material such as bFeCo and has perpendicular magnetic anisotropy in the thickness direction.

磁気ディスク7の例えば本例では図中下側に、光源を備
えた光供給手段(不図示)から供給される光ど−ムBを
集束させ磁気ディスク7上に微小スポラi・状に絞り込
んで照射する対物レンズ1゜が配設されている。この対
物レンズ1oは基体11により保持され、この基体11
には磁気ディスク7に対しその厚さ方向の垂直外部磁界
を付与する磁気コイル12が装着され、光ヘツド部Hが
構成されている。更に基体11には、この光ヘツド部H
を一体に所定の方向に走査させるアクチュエータ13が
設けられており、本例においては光ヘツド部Hを磁気デ
ィスク7の半径方向に所定距離を段階的に走査させる。
For example, in this example, on the lower side of the magnetic disk 7 in the figure, an optical beam B supplied from a light supply means (not shown) equipped with a light source is focused and squeezed onto the magnetic disk 7 into a minute spora I shape. A 1° objective lens for irradiation is provided. This objective lens 1o is held by a base 11, and this base 11
A magnetic coil 12 is attached to the magnetic disk 7 to apply an external magnetic field perpendicular to the thickness direction of the magnetic disk 7, thereby forming an optical head section H. Furthermore, this optical head portion H is provided on the base body 11.
An actuator 13 is provided which causes the optical head section H to scan the magnetic disk 7 in a predetermined direction in a stepwise manner in the radial direction of the magnetic disk 7.

又、アクチュエータ13には、光ヘツド部Hと磁気ディ
スク7の間隔Wを高精度で一定距離に制御するサーボm
構が内設され、前述したオートフォーカス機構の効果が
発揮される構成となっている。即ち、磁気ディスク7表
面の微妙な上下動や凹凸を鋭敏に検知して光ヘツド部H
の位置をフィードバック制御し、双方の間隔Wを高精度
で一定距離に維持する。尚、光源(不図示)としては、
A−rレーザ、He−Neレーザ又は半導体レーザ等の
レーザ光が好適である。
The actuator 13 also includes a servo m that controls the distance W between the optical head H and the magnetic disk 7 to a constant distance with high precision.
The autofocus mechanism is installed internally, and is configured to take advantage of the effects of the autofocus mechanism described above. That is, by sensitively detecting subtle vertical movements and irregularities on the surface of the magnetic disk 7, the optical head section H
The position is feedback-controlled, and the distance W between the two is maintained at a constant distance with high precision. In addition, as a light source (not shown),
Laser light such as an Ar laser, a He-Ne laser, or a semiconductor laser is suitable.

而して、光ヘツド部Hの磁気ディスク7を挾んで反対側
には、補助磁極14が配設されている。
An auxiliary magnetic pole 14 is disposed on the opposite side of the optical head H with the magnetic disk 7 interposed therebetween.

補助磁極14は、第3図に示される如く、軟磁性体を材
料として薄片状に形成されており、その長手方向端面1
4aを磁気ディスク7に対向させると共にその長手方向
を磁気ディスク7の半径方向即ち光ヘツド部Hの走査方
向に沿って延在させる態様で設置されている。ここで、
厚さ寸法aは磁気ディスク7を挾んで対向覆る磁気コイ
ル12の磁極面12aの直径りより十分に小さく、また
、長さ寸法ρは少くとも磁気ディスク7の記録部分7′
の半径方向幅Pより長くなるように、補助磁極14を形
成する必要がある、かくの如く補助磁極14を構成する
ことにより、磁気コイル12により付与される磁界が弱
い場合でも磁束密度の高い強い磁界を磁気ディスク7の
厚さ方向に形成することが可能となる。即ち、記録ヘッ
ド部を正面と側面から視た第4図及び第5図で示される
如く、−磁気コイル12から発した磁力線は磁気ディス
ク7を透過して反対側の補助磁極14の端面14aに集
束される為、第6図で示される補助磁極14を設けない
場合に比べて、磁気ディスク7の所望の目標区域、即ち
スポット照射部分に、より磁束密度が高くかつ厚さ方向
に沿って均一な磁界を形成することができる。従って、
磁界発生手段としての磁気コイル12の導線の巻数を減
らし小型化することが可能となり、これにより光ヘツド
部Hの重量が軽減されその磁気ディスク7表面に対する
追従性が向上される。又、第5図に示される如く、図中
上下方向に磁力線が集中される為磁気ディスク7表面の
上下動や凹凸に対しても影響されず安定して均一な磁界
が付与される。これにより、補助磁極14の磁気ディス
ク7との相対位置変化に対応して磁界を調整しなくても
常時正確に均一なビットを形成することが可能となる。
As shown in FIG. 3, the auxiliary magnetic pole 14 is formed into a thin piece of soft magnetic material, and its longitudinal end surface 1
The optical head 4a is arranged so as to face the magnetic disk 7 and to extend its longitudinal direction along the radial direction of the magnetic disk 7, that is, the scanning direction of the optical head section H. here,
The thickness dimension a is sufficiently smaller than the diameter of the magnetic pole surface 12a of the magnetic coil 12 that covers and sandwiches the magnetic disk 7, and the length dimension ρ is at least the recording portion 7' of the magnetic disk 7.
It is necessary to form the auxiliary magnetic pole 14 so that it is longer than the radial width P of It becomes possible to form a magnetic field in the thickness direction of the magnetic disk 7. That is, as shown in FIGS. 4 and 5, when the recording head section is viewed from the front and side, - the lines of magnetic force emitted from the magnetic coil 12 pass through the magnetic disk 7 and reach the end surface 14a of the auxiliary magnetic pole 14 on the opposite side. Since the magnetic flux is focused, the magnetic flux density is higher and more uniform in the thickness direction in the desired target area of the magnetic disk 7, that is, in the spot irradiation area, than in the case where the auxiliary magnetic pole 14 shown in FIG. 6 is not provided. A strong magnetic field can be created. Therefore,
It is possible to reduce the number of windings of the conductive wire of the magnetic coil 12 as a magnetic field generating means, thereby reducing the weight of the optical head H and improving its ability to follow the surface of the magnetic disk 7. Further, as shown in FIG. 5, since the lines of magnetic force are concentrated in the vertical direction in the figure, a stable and uniform magnetic field is applied without being affected by vertical movement or unevenness of the surface of the magnetic disk 7. This makes it possible to always accurately form uniform bits without adjusting the magnetic field in response to changes in the relative position of the auxiliary magnetic pole 14 with respect to the magnetic disk 7.

更に又、磁気コイル12の小型化により、発生する熱や
磁界の悪影響が軽減されてオートフォーカス機構の精度
が向上し、より高精度な光磁気記録処理が可能となる。
Furthermore, by reducing the size of the magnetic coil 12, the adverse effects of the generated heat and magnetic field are reduced, the accuracy of the autofocus mechanism is improved, and more accurate magneto-optical recording processing becomes possible.

以上の如く構成された本実施例の動作について、以下に
説明する。
The operation of this embodiment configured as described above will be explained below.

入力される情報に従い変調されて出力された例えばl−
1e−NeレーザビームBは、各種ミラー等の光学要素
を経て対物レンズ10に供給される。
For example, l-
The 1e-Ne laser beam B is supplied to the objective lens 10 through optical elements such as various mirrors.

対物レンズ10に入射したレーザビームBは、ここで集
束され磁気ディスク7上に微小スポット状に絞り込まれ
て照射される。これにより、微小スポットの照射部分は
選択的に温度が上昇して抗磁力が低下する。然るに、こ
の微小スポットの照射部分Sには、磁気コイル12と補
助磁極14が協働してその厚さ方向に沿って均一な磁界
を形成している。従って、磁気ディスク7の照射部分S
のみが選択的に外部磁界の方向に沿って磁化され、微小
なビットが形成される。この場合、重量軽減された光ヘ
ツド部Hはオートフォーカス機構により高精度で位置制
御され、照射するスポラt−Sの大きさを常時一定に維
持する。又、照射部分Sには高密度に集束された外部磁
界が均一に付与されている。従って、磁気ディスク7表
面の微妙な上下動や凹凸に拘わらず、安定して極めて正
確なビットの形成が実施される。
The laser beam B incident on the objective lens 10 is focused there and is focused onto the magnetic disk 7 in the form of a minute spot. As a result, the temperature of the irradiated portion of the micro spot increases selectively, and the coercive force decreases. However, in the irradiated portion S of this minute spot, the magnetic coil 12 and the auxiliary magnetic pole 14 cooperate to form a uniform magnetic field along the thickness direction. Therefore, the irradiated portion S of the magnetic disk 7
are selectively magnetized along the direction of the external magnetic field, forming tiny bits. In this case, the position of the light head H whose weight has been reduced is controlled with high precision by an autofocus mechanism, and the size of the irradiated spora t-S is always maintained constant. Further, a highly concentrated external magnetic field is uniformly applied to the irradiated portion S. Therefore, bits can be stably and extremely accurately formed regardless of slight vertical movements or irregularities on the surface of the magnetic disk 7.

この様にして、磁気ディスク7が1回転する間に1周り
コース(1トラツク)のビット形成が実施されると、光
ヘツド部Hが磁気ディスク7の半径方向に1トラツク分
だけ走査し新たなトラックへのビット形成が開始される
。以上の如くして、入力情報に応じた微小ビットが磁気
ディスクンの記録部分7′に高密度で正確に形成され、
情報の記録が完゛了する。
In this way, when the bit formation for one round course (one track) is performed during one rotation of the magnetic disk 7, the optical head H scans one track in the radial direction of the magnetic disk 7 and creates a new bit. Bit formation on the track begins. As described above, minute bits corresponding to the input information are accurately formed in the recording portion 7' of the magnetic disc with high density.
Recording of information is completed.

尚、上記実施例においては、光ヘツド部Hの走査全領域
に対応可能な長い磁極面を有する補助磁極を固設したが
、これに限らず補助磁極を光ヘツド部Hと記録媒体を介
して対向させたまま双方が同期して所定方向に走査する
構成としても良い。
In the above embodiment, an auxiliary magnetic pole having a long magnetic pole surface that can cover the entire scanning area of the optical head H is fixed, but the auxiliary magnetic pole is not limited to this. It is also possible to have a configuration in which both of them are left facing each other and scan in a predetermined direction in synchronization.

又、本発明は、光ヘツド部Hを記録と再生に兼用するヘ
ッドとして使用する光磁気記録再生装置にも適用可能で
ある。
Further, the present invention is also applicable to a magneto-optical recording/reproducing apparatus in which the optical head section H is used as a head for both recording and reproduction.

効  果 以上詳述した如く、本発明によれば、薄片状の補助磁極
を光ヘツド部の磁界発生手段に記録媒体を挾んで対向配
置させることにより、磁界発生手段が小型化され光ヘツ
ド部重量が軽減されてオートフォーカス機能が向上する
。又、磁界発生手段が発生させる熱や磁界のオートフォ
ーカス機構への悪影響も抑制される。更に、形成される
外部磁界が記録媒体の厚さ方向に沿って高密度に形成さ
れる。従って記録媒体のスポット照射部分の温度分布及
び磁界が高精度で常時均一に保持され、正確なビットの
形成、即ち、光磁気記録再生処理を安定的に実施するこ
とが可能となる。尚、本発明は上記の特定の実施例に限
定されるべきものではなく、本発明の技術的範囲におい
て種々の変形が可能であることは勿論である。
Effects As detailed above, according to the present invention, by arranging the flaky auxiliary magnetic pole to face the magnetic field generating means of the optical head section with the recording medium sandwiched therebetween, the magnetic field generating means can be miniaturized and the weight of the optical head section can be reduced. is reduced, improving autofocus function. Further, the adverse effects of the heat and magnetic field generated by the magnetic field generating means on the autofocus mechanism are also suppressed. Furthermore, the external magnetic field is formed with high density along the thickness direction of the recording medium. Therefore, the temperature distribution and magnetic field of the spot irradiated portion of the recording medium are kept uniform at all times with high precision, making it possible to form accurate bits, that is, to stably perform magneto-optical recording and reproducing processing. It should be noted that the present invention should not be limited to the specific embodiments described above, and it goes without saying that various modifications can be made within the technical scope of the present invention.

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

第1図は従来の光磁気記録再生装置を示した模式図、第
2図は本発明の1実施例を示した模式図、第3図は補助
磁極11を示した斜視図、第4図。 第5図は夫々本発明の1実施例°の記録ヘッド部を示し
た正面図と側面図、第6図は従来の記録ヘッド部を示し
た正面図である。 (符号の説明) 1.7: 磁気ディスク 4.10:  対物レンズ 5.12:  !1気コイル 14: 補助Fi1極 第11J 第 3 1゛ユ、1
FIG. 1 is a schematic diagram showing a conventional magneto-optical recording/reproducing device, FIG. 2 is a schematic diagram showing an embodiment of the present invention, FIG. 3 is a perspective view showing an auxiliary magnetic pole 11, and FIG. FIG. 5 is a front view and a side view showing a recording head section according to an embodiment of the present invention, respectively, and FIG. 6 is a front view showing a conventional recording head section. (Explanation of symbols) 1.7: Magnetic disk 4.10: Objective lens 5.12: ! 1st coil 14: Auxiliary Fi1 pole No. 11J No. 3 1゛yu, 1

Claims (1)

【特許請求の範囲】 1、磁気異方性を備えた磁性薄膜からなる記録媒体と、
光源を備えた光供給手段と、前記光供給手段から供給さ
れた光を前記磁性薄膜にスポット状に集束させる集光手
段と、前記集光手段と一体移動可能に配設され前記磁性
[!に磁界を付与する磁界発生手段と、前記磁界発生手
段と前記記録媒体を挾んで反対側に互いに対向すべく配
設された補助磁極とを有し、前記補助磁極の対向磁極面
の幅寸法が前記磁界発生手段の対向磁極面の前記幅寸法
に対応する寸法より充分小さいことを特徴とする光磁気
記録発生装置。 2、上記第1項に於いて、前記補助磁極は前記対向磁極
面の長手方向を前記磁界発生手段の移動方向に延在させ
て固設されると共に前記長手方向寸法は少なくとも前記
記録媒体に於ける前記集光手段によるスポット照射領域
の長手方向長さより長いことを特徴とする光磁気記録再
生装置。
[Claims] 1. A recording medium comprising a magnetic thin film with magnetic anisotropy;
A light supply means including a light source; a condensing means for focusing the light supplied from the light supply means on the magnetic thin film in a spot shape; and an auxiliary magnetic pole disposed to face each other on opposite sides sandwiching the magnetic field generating means and the recording medium, the width dimension of the opposing magnetic pole surface of the auxiliary magnetic pole being A magneto-optical recording generator characterized in that a dimension corresponding to the width dimension of the opposing magnetic pole surface of the magnetic field generating means is sufficiently smaller. 2. In the above item 1, the auxiliary magnetic pole is fixed so that the longitudinal direction of the opposing magnetic pole surface extends in the moving direction of the magnetic field generating means, and the longitudinal dimension is at least as large as that of the recording medium. A magneto-optical recording/reproducing device characterized in that the length is longer than the length in the longitudinal direction of the spot irradiation area by the light condensing means.
JP5367983A 1983-03-31 1983-03-31 Optical magnetic recording and reproducing device Pending JPS59180802A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5367983A JPS59180802A (en) 1983-03-31 1983-03-31 Optical magnetic recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5367983A JPS59180802A (en) 1983-03-31 1983-03-31 Optical magnetic recording and reproducing device

Publications (1)

Publication Number Publication Date
JPS59180802A true JPS59180802A (en) 1984-10-15

Family

ID=12949502

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5367983A Pending JPS59180802A (en) 1983-03-31 1983-03-31 Optical magnetic recording and reproducing device

Country Status (1)

Country Link
JP (1) JPS59180802A (en)

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