JPS62189653A - Photomagnetic recording and reproducing head - Google Patents

Photomagnetic recording and reproducing head

Info

Publication number
JPS62189653A
JPS62189653A JP3071086A JP3071086A JPS62189653A JP S62189653 A JPS62189653 A JP S62189653A JP 3071086 A JP3071086 A JP 3071086A JP 3071086 A JP3071086 A JP 3071086A JP S62189653 A JPS62189653 A JP S62189653A
Authority
JP
Japan
Prior art keywords
magnetic field
magneto
recording medium
optical recording
electromagnets
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
JP3071086A
Other languages
Japanese (ja)
Inventor
Toshiaki Iwanaga
敏明 岩永
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP3071086A priority Critical patent/JPS62189653A/en
Publication of JPS62189653A publication Critical patent/JPS62189653A/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
    • G11B11/10534Heads for recording by magnetising, demagnetising or transfer of magnetisation, by radiation, e.g. for thermomagnetic recording
    • G11B11/10536Heads for recording by magnetising, demagnetising or transfer of magnetisation, by radiation, e.g. for thermomagnetic recording using thermic beams, e.g. lasers

Landscapes

  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To produce a magnetic field vertical to the film surface of a photomagnetic recording medium in a sharp and intensive way in terms of space, by using >=2 pieces of electromagnets contains magnetic cores set opposite to each other as the external magnetic field generating means and conducting the current to the coils so that the same polarities are set opposite to each other. CONSTITUTION:The coils containing magnetic cores, i.e., the electromagnets 20 and 21 are set opposite to each other as the external magnetic field generating means. Here a gap space between both magnets 20 and 21 is decided so that the luminous flux given from an objective lens 9 can pass through said gap. Then the current is conducted to both coils so that the same polarities of both magnets 20 and 21 are set opposite to each other. As a result, a sharp vertical magnetic field is obtained in terms of space between both electrodes 20 and 21. Thus it is possible to produce a magnetic field vertical to the film surface of a photomagnetic recording medium 10 in a sharp and intensive way in terms of space.

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媒体を用いた光磁気記録再生へノド
に関するもので、特に記録、消去時の外部磁界不足を補
い局所的に磁界の収束を容易に行うことのできる構成を
持つ外部磁界発生手段を搭載した光磁気記録再生ヘッド
に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a magneto-optical recording and reproducing device using a magneto-optical recording medium, and in particular, it compensates for the lack of external magnetic field during recording and erasing, and locally increases the magnetic field. The present invention relates to a magneto-optical recording/reproducing head equipped with external magnetic field generating means having a configuration that allows easy convergence.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来より光磁気メモリの記録媒体としては、MnB1.
  MnAlGe、  PtCo、  GdFe、  
GdCo、TbFe、GdTbFe等の材料が用いられ
ている。第6図に、このような材料が用いられる光磁気
メモリすなわち光磁気記録媒体の基本的構成を示す。光
磁気メモリは、ガラスやシリコンウェハー等の基板lの
上に、光磁気記録用の記録媒体め薄膜を記録層として、
例えば真空蒸着法やスパッタリング等の方法で形成する
ことにより得られる。これらの記録媒体の特性として、
膜面に垂直な磁気異方性を有し、キュリ一温度および磁
気補償温度が比較的低いなどの特性がある。これらの記
録媒体は垂直磁気異方性を有しているので、情報の記録
としては、第6図に示すように基板1上の記録層2の膜
面に垂直な上向き磁化3か下向き磁化4かで情報をそれ
ぞれO”、“l”のディジタル信号としての2値で書き
込むことにより行われる。情報の記録の方法としては、
例えば予め記録層2の膜面全体に垂直に外部磁界をかけ
、上向き磁化となるように記録層を磁化させて“0”を
書き込んだ後、“l”を書き込む部分にレーザビームを
スポット的に照射して加熱する。
Conventionally, as a recording medium for magneto-optical memory, MnB1.
MnAlGe, PtCo, GdFe,
Materials such as GdCo, TbFe, and GdTbFe are used. FIG. 6 shows the basic structure of a magneto-optical memory, ie, a magneto-optical recording medium, in which such a material is used. Magneto-optical memory uses a thin film as a recording medium for magneto-optical recording as a recording layer on a substrate such as glass or silicon wafer.
For example, it can be formed by a method such as vacuum evaporation or sputtering. As the characteristics of these recording media,
It has characteristics such as having magnetic anisotropy perpendicular to the film surface, and relatively low Curie temperature and magnetic compensation temperature. Since these recording media have perpendicular magnetic anisotropy, information can be recorded using either upward magnetization 3 or downward magnetization 4 perpendicular to the film surface of the recording layer 2 on the substrate 1, as shown in FIG. This is done by writing information in binary form as digital signals of "O" and "l" respectively.As a method of recording information,
For example, apply an external magnetic field perpendicularly to the entire film surface of the recording layer 2 in advance, magnetize the recording layer so that it is magnetized upward, and write "0", and then apply a spot laser beam to the part where "l" is to be written. Irradiate and heat.

加熱された微小部分は保磁力1(cが小さくなり、レー
ザビーム照射の際微弱な外部磁界を下向き磁化となる方
向に与えておくと、磁化反転して“1”が記録される。
The coercive force 1 (c) of the heated minute portion becomes small, and if a weak external magnetic field is applied in the direction of downward magnetization during laser beam irradiation, the magnetization is reversed and "1" is recorded.

このように、レーザビームを照射するかしないかにより
、記録層2に磁気記録パターンを形成する方法がとられ
る。また、情報の読み出しの方法としては、例えば直線
偏光したレーザビームを前記磁気記録パターンに照射し
た場合、その反射光または透過光の偏光面を回転させる
効果(それぞれ磁気カー効果、磁気ファラデー効果と呼
ばれる)を記録層2は有しているので、例えば磁気カー
効果を利用する場合には、反射光の偏光面の回転角θK
が記録磁気化の方向によって異なることを利用して、反
射光が光検出器に入る前に検光子を通し、磁化の向きに
対応した情報を光量変化として読み出す。また、すでに
情報が記録されている記録媒体に新しい情報を書き込む
ときには、まず媒体面に垂直に記録媒体の保磁力Hcよ
り小さな外部磁界をかけ記録用トラックの記録する部分
の始端から終端までレーザビームを走査加熱し、記録媒
体の保磁力Hcを低下させて記録媒体の磁化をすべて周
囲の磁界と同じ方向に向ける。これが消去に相当する。
In this way, a method is used to form a magnetic recording pattern on the recording layer 2 depending on whether or not to irradiate the laser beam. In addition, as a method of reading information, for example, when the magnetic recording pattern is irradiated with a linearly polarized laser beam, the effect of rotating the plane of polarization of the reflected light or transmitted light (called the magnetic Kerr effect and magnetic Faraday effect, respectively) is known. ), the recording layer 2 has, for example, when using the magnetic Kerr effect, the rotation angle θK of the polarization plane of the reflected light
Taking advantage of the fact that the amount of light differs depending on the direction of recording magnetization, the reflected light is passed through an analyzer before entering the photodetector, and information corresponding to the direction of magnetization is read out as a change in the amount of light. When writing new information to a recording medium on which information has already been recorded, first an external magnetic field smaller than the coercive force Hc of the recording medium is applied perpendicular to the medium surface and a laser beam is applied from the beginning to the end of the recording section of the recording track. is scanned and heated to lower the coercive force Hc of the recording medium and direct all the magnetization of the recording medium in the same direction as the surrounding magnetic field. This corresponds to erasure.

次に消去とは逆方向の外部磁界をかけ、すでに述べた原
理により新しい情報を書き込む。
Next, an external magnetic field is applied in the direction opposite to that for erasing, and new information is written using the principle already described.

以上のようにして光磁気記録媒体は消去と書き換えが自
由に行えることが大きな特徴である。この情報の記録、
再生、消去には外部磁界の作用が大きく関与している。
A major feature of the magneto-optical recording medium is that it can be freely erased and rewritten as described above. Recording this information;
Reproduction and erasing are largely influenced by the action of external magnetic fields.

外部磁界としては光磁気記録媒体に対して垂直な一様磁
界であるのが望ましく、結果的に再生CN比が飽和傾向
を示す磁界強度である必要がある。
It is desirable that the external magnetic field be a uniform magnetic field perpendicular to the magneto-optical recording medium, and as a result, the magnetic field strength must be such that the reproduction CN ratio tends to be saturated.

従来、外部磁界発生手段としては、永久磁石を用いる方
法、電磁石を用いる方法が考えられる。
Conventionally, as external magnetic field generating means, methods using permanent magnets and methods using electromagnets can be considered.

永久磁石を用いる方法では、記録と消去の場合とで磁界
の向きを反転させるため空間的に永久磁石の向きを変え
る必要があり機械的な構成が必要であるといった欠点を
持つ。また、永久磁石では光磁気記録媒体からの距離を
変化させることで磁界強度をコントロールしなければな
らないといった欠点を持つ。さらに永久磁石では常に磁
界を発生しているため、光磁気記録媒体としては高い保
磁力Hcを持つ必要があるといった制約もある。他方、
電磁石を用いる方法では永久磁石の持つ欠点を解消する
ことが可能である。しかしながら、再生CN比が飽和傾
向を示す以上の磁界強度を発生するには従来の簡単な電
磁石では大きな寸法を要し、大きな電流を流す必要があ
った。また、従来の簡単な電磁石では高速のスイッチン
グ動作ができないため、磁気記録で行われている重ね書
き記録ができないといった欠点を有している。
The method using permanent magnets has the disadvantage that it is necessary to change the direction of the permanent magnet spatially in order to reverse the direction of the magnetic field between recording and erasing, and a mechanical configuration is required. Additionally, permanent magnets have the disadvantage that the magnetic field strength must be controlled by changing the distance from the magneto-optical recording medium. Furthermore, since permanent magnets always generate a magnetic field, there is a restriction that a magneto-optical recording medium must have a high coercive force Hc. On the other hand,
The method using electromagnets can overcome the drawbacks of permanent magnets. However, in order to generate a magnetic field strength above which the reproduced CN ratio shows a tendency to saturate, a conventional simple electromagnet requires a large size and requires a large current to flow. Furthermore, because conventional simple electromagnets cannot perform high-speed switching operations, they have the disadvantage that they cannot perform overwrite recording, which is done in magnetic recording.

本発明の目的は前述の如き欠点を改善して、情報の記録
、消去時の外部磁界を小さな電流で発生でき、しかも高
速のスイッチング動作が可能な外部磁界発生手段を搭載
した光磁気記録再生ヘッドを提供することにある。
The object of the present invention is to improve the above-mentioned drawbacks, and to provide a magneto-optical recording/reproducing head which is equipped with an external magnetic field generating means capable of generating an external magnetic field with a small current when recording and erasing information, and capable of high-speed switching operation. Our goal is to provide the following.

c問題点を解決するだめの手段〕 本発明は、レーザを光源とし、光源から発した光束を光
磁気記録媒体面上に築光照射し光磁気的に情報を記録再
生する光磁気記録再生ヘッドにおいて、前記光束を囲む
ように同じ極性の磁極を対向させて配置した2個以上の
電磁石よりなる外部磁界発生手段をヘッド前面に設置し
たことを特徴とする光磁気記録再生ヘッド。
Solution to Problem c] The present invention provides a magneto-optical recording and reproducing head that uses a laser as a light source and irradiates a light flux emitted from the light source onto the surface of a magneto-optical recording medium to optically record and reproduce information. A magneto-optical recording/reproducing head, characterized in that external magnetic field generating means comprising two or more electromagnets arranged with magnetic poles of the same polarity facing each other so as to surround the light flux is installed on the front surface of the head.

〔実施例〕〔Example〕

次に本発明の実施例を図面を参照して説明する。 Next, embodiments of the present invention will be described with reference to the drawings.

第1図は本発明の光磁気記録再生ヘッドの一実施例を示
す。この光磁気記録再生ヘッドは、レーザを光源として
対物レンズを含むアクチュエータ前面に本発明に係る外
部磁界発生手段である電磁石を設けた構成である。但し
、ここではアクチュエータ駆動用の制御信号を得る光学
系については省略しである。
FIG. 1 shows an embodiment of the magneto-optical recording/reproducing head of the present invention. This magneto-optical recording/reproducing head has a structure in which a laser is used as a light source and an electromagnet, which is an external magnetic field generating means according to the present invention, is provided in front of an actuator including an objective lens. However, the optical system for obtaining the control signal for driving the actuator is omitted here.

光源としては例えば半導体レーザ5を用いる。For example, a semiconductor laser 5 is used as the light source.

レーザ5より発生した光束は、コリメートレンズ6、ビ
ームスプリッタ7の順に透過し、アクチュエータ8に設
置された対物レンズ9により光磁気記録媒体10上に築
光照射される。なお、光磁気記録媒体10は、レーザに
対し透明な基板11上に形成されている。集光照射され
た光束の一部が記録媒体10により反射される。その反
射光束をビームスプリッタフにより光分割し、2分の1
波長板12により光束の偏光面をπ/4だけ回転させ、
検光子13により光束を2分割し、集光レンズ14.1
5で光検出器16.17に導くといった構成である。本
実施例では、アクチュエータ8前面には、光束が通過で
きる分の空間(ギャップ間隔)を持たせた本発明に係る
外部磁界発生手段18が設けである。この外部磁界発生
手段が発生する外部磁界としては、 (1)光磁気記録媒体10上に集光照射される部分で膜
面に垂直な磁界分布が存在すること、(2)外部磁界の
強さが再生CN比の飽和状態を示す以上の大きさがある
こと、 が必要である。この2つの条件を達成できる電磁石とし
ては空心ソレノイドが考えられる。しかしながら、空心
ソレノイドでは小電流での発生磁界強度が限られる。 
そこで、本実施例では外部磁界発生手段として第2図で
示すように磁心入りのコイル、すなわち電磁石20.2
1を対向させて配置する。この場合、ギャップ間隔は、
第1図の対物レンズ9からの光束が通過し得るように選
ばれる。そして、各々の電磁石には互いに同じ極性が対
向するようにコイルに電流を流す。本実施例ではN極が
互(、Nに対向するものとする。
The light beam generated by the laser 5 passes through a collimating lens 6 and a beam splitter 7 in this order, and is irradiated onto a magneto-optical recording medium 10 by an objective lens 9 installed on an actuator 8 . Note that the magneto-optical recording medium 10 is formed on a substrate 11 that is transparent to laser. A part of the focused light beam is reflected by the recording medium 10. The reflected light beam is split into two parts by a beam splitter.
The polarization plane of the light beam is rotated by π/4 by the wave plate 12,
The light beam is divided into two by the analyzer 13, and the condensing lens 14.1
5 leads to photodetectors 16 and 17. In this embodiment, an external magnetic field generating means 18 according to the present invention is provided on the front surface of the actuator 8 and has a space (gap interval) for a light beam to pass through. The external magnetic field generated by this external magnetic field generating means includes: (1) the presence of a magnetic field distribution perpendicular to the film surface in the portion of the magneto-optical recording medium 10 that is irradiated with focused light; and (2) the strength of the external magnetic field. It is necessary that the value is larger than that indicating the saturated state of the reproduced CN ratio. An air-core solenoid can be considered as an electromagnet that can achieve these two conditions. However, with air-core solenoids, the strength of the generated magnetic field at small currents is limited.
Therefore, in this embodiment, as an external magnetic field generating means, as shown in FIG.
1 are placed facing each other. In this case, the gap spacing is
It is selected so that the light beam from the objective lens 9 in FIG. 1 can pass therethrough. Then, current is passed through the coils of each electromagnet so that the same polarity faces each other. In this embodiment, it is assumed that the N poles are opposite to each other (and N).

第3図にこれらの2つの電磁石20.21がら出る磁力
線の様子を示す。このように、同じ極性側を対向させる
ことにより、第4図に示すように電磁石20.21の中
間では(第3図および第4図では光軸を点線で示してい
る)空間的に鋭い垂直磁界が得られる。従って、光磁気
記録媒体1゜の膜面に垂直な磁界を空間的に鋭く、しが
も強く発生させることが可能となる。
FIG. 3 shows the lines of magnetic force coming out of these two electromagnets 20 and 21. In this way, by arranging the same polarity sides to face each other, as shown in FIG. A magnetic field is obtained. Therefore, it is possible to generate a spatially sharp and strong magnetic field perpendicular to the 1° film surface of the magneto-optical recording medium.

以上の実施例では、2個の電磁石で構成したが、それよ
り多くの個数の電磁石で構成してもよい。
In the above embodiment, two electromagnets were used, but a larger number of electromagnets may be used.

第5図は4個の電磁石を用いた外部磁界発生手段の平面
図である。4個の電磁石22,23,24゜25は、通
過する光束を囲むように互いに直交する位置に配置され
ている。そして、これら電磁石のコイルには、互いに同
じ極性の磁極が対向するように電流を流す。本実施例に
おいても、これら電磁石の中間では空間的に鋭い垂直磁
界が得られる。このように多数の電磁石を用いれば、同
じ磁界強度を得るのに1個当たりに流す電流を減少させ
ることができ、高速なスイッチング動作が可能となる。
FIG. 5 is a plan view of an external magnetic field generating means using four electromagnets. The four electromagnets 22, 23, 24.degree. 25 are arranged at mutually orthogonal positions so as to surround the passing light beam. Then, current is passed through the coils of these electromagnets so that the magnetic poles of the same polarity face each other. In this embodiment as well, a spatially sharp vertical magnetic field is obtained between these electromagnets. If a large number of electromagnets are used in this way, the current flowing per electromagnet can be reduced to obtain the same magnetic field strength, and high-speed switching operation becomes possible.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明の光磁気記録再生ヘッドによ
れば、外部磁界発生手段として2個以上の磁心入すの電
磁石を対向させて配置し、同じ極性が対向するようにコ
イルに電流番流すことによ・り光磁気記録媒体の膜面に
垂直な磁界を、空間的に鋭く、しかも強く発生させるこ
とが可能である。
As explained above, according to the magneto-optical recording/reproducing head of the present invention, two or more electromagnets with magnetic cores are arranged facing each other as external magnetic field generating means, and current is passed through the coils so that the same polarity faces each other. As a result, it is possible to generate a spatially sharp and strong magnetic field perpendicular to the film surface of the magneto-optical recording medium.

従って、再生CN比の飽和傾向を示す磁界強度を従来の
電磁石に比べ、小さな電流で得るこが可能となる。また
、多数の対向電磁石を用いれば、1個当たりに流す電流
を減少させることができるため、高速での磁界のスイッ
チング動作が可能となり、重ね書き記録を容易に達成で
きる。さらには、外部磁界発生手段をアクチュエータ前
面に設けることにより、光磁気記録再生装置自体を小型
化できる。
Therefore, it is possible to obtain the magnetic field strength that indicates the saturation tendency of the reproduced CN ratio with a smaller current than with conventional electromagnets. Furthermore, if a large number of opposing electromagnets are used, the current flowing per electromagnet can be reduced, so that high-speed magnetic field switching operation is possible, and overwriting recording can be easily achieved. Furthermore, by providing the external magnetic field generating means in front of the actuator, the magneto-optical recording/reproducing apparatus itself can be made smaller.

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

第1図は本発明の光磁気記録再生ヘッドの一実施例を示
す図、 第2図は本発明に係る外部磁界発生手段である対向する
電磁石の第1の例を示す図、 第3図は第2図で示す電磁石から発生する磁力線の様子
を説明する図、 第4図は第2図で示す電磁石から発生ずる磁界強度分布
を説明する図、 第5図は本発明に係る外部磁界発生手段である対向する
電磁石の第2の例の平面図、 第6図は光磁気記録媒体の基本構成を示す図である。 5・・・・・半導体レーザ 6・・・・・コリメータレンズ 7・・・・・ビームスプリッタ 8・・・・・アクチュエーダ 9・・・・・対物レンズ 10・・・・・光磁気記録媒体 11・・・・・基板 12・・・・・2分の1波長板 13・・・・・検光子 14、15  ・・・築光レンズ 16、17  ・・・光検出器 18・・・・・外部磁界発生手段 20〜25・・・電磁石
FIG. 1 is a diagram showing an embodiment of the magneto-optical recording/reproducing head of the present invention, FIG. 2 is a diagram showing a first example of opposing electromagnets which are external magnetic field generating means according to the present invention, and FIG. FIG. 2 is a diagram explaining the magnetic field lines generated from the electromagnet shown in FIG. 2. FIG. 4 is a diagram explaining the magnetic field intensity distribution generated from the electromagnet shown in FIG. 2. FIG. 5 is an external magnetic field generating means according to the present invention. FIG. 6 is a plan view of a second example of opposing electromagnets. FIG. 6 is a diagram showing the basic configuration of a magneto-optical recording medium. 5... Semiconductor laser 6... Collimator lens 7... Beam splitter 8... Actuator 9... Objective lens 10... Magneto-optical recording medium 11 ... Substrate 12 ... Half wavelength plate 13 ... Analyzers 14, 15 ... Light-building lenses 16, 17 ... Photodetector 18 ... External magnetic field generating means 20 to 25...electromagnet

Claims (1)

【特許請求の範囲】[Claims] (1)レーザを光源とし、光源から発した光束を光磁気
記録媒体面上に集光照射し光磁気的に情報を記録再生す
る光磁気記録再生ヘッドにおいて、前記光束を囲むよう
に同じ極性の磁極を対向させて配置した2個以上の電磁
石よりなる外部磁界発生手段をヘッド前面に設置したこ
とを特徴とする光磁気記録再生ヘッド。
(1) In a magneto-optical recording/reproducing head that uses a laser as a light source and condenses and irradiates a light beam emitted from the light source onto the surface of a magneto-optical recording medium to optically record and reproduce information, a light beam of the same polarity surrounds the light beam. 1. A magneto-optical recording/reproducing head characterized in that external magnetic field generating means comprising two or more electromagnets with magnetic poles facing each other is installed on the front surface of the head.
JP3071086A 1986-02-17 1986-02-17 Photomagnetic recording and reproducing head Pending JPS62189653A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3071086A JPS62189653A (en) 1986-02-17 1986-02-17 Photomagnetic recording and reproducing head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3071086A JPS62189653A (en) 1986-02-17 1986-02-17 Photomagnetic recording and reproducing head

Publications (1)

Publication Number Publication Date
JPS62189653A true JPS62189653A (en) 1987-08-19

Family

ID=12311203

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3071086A Pending JPS62189653A (en) 1986-02-17 1986-02-17 Photomagnetic recording and reproducing head

Country Status (1)

Country Link
JP (1) JPS62189653A (en)

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